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WO2006006630A1 - Magnetoresistive device, method for manufacturing magnetoresistive device and magnetic random access memory - Google Patents

Magnetoresistive device, method for manufacturing magnetoresistive device and magnetic random access memory Download PDF

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Publication number
WO2006006630A1
WO2006006630A1 PCT/JP2005/012955 JP2005012955W WO2006006630A1 WO 2006006630 A1 WO2006006630 A1 WO 2006006630A1 JP 2005012955 W JP2005012955 W JP 2005012955W WO 2006006630 A1 WO2006006630 A1 WO 2006006630A1
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Prior art keywords
layer
ferromagnetic layer
tunnel barrier
manufacturing
effect element
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French (fr)
Japanese (ja)
Inventor
Hiroaki Honjo
Yoshiyuki Fukumoto
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NEC Corp
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NEC Corp
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    • BPERFORMING OPERATIONS; TRANSPORTING
    • B82NANOTECHNOLOGY
    • B82YSPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
    • B82Y25/00Nanomagnetism, e.g. magnetoimpedance, anisotropic magnetoresistance, giant magnetoresistance or tunneling magnetoresistance
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B82NANOTECHNOLOGY
    • B82YSPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
    • B82Y40/00Manufacture or treatment of nanostructures
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/02Measuring direction or magnitude of magnetic fields or magnetic flux
    • G01R33/06Measuring direction or magnitude of magnetic fields or magnetic flux using galvano-magnetic devices
    • G01R33/09Magnetoresistive devices
    • G01R33/093Magnetoresistive devices using multilayer structures, e.g. giant magnetoresistance sensors
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11CSTATIC STORES
    • G11C11/00Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor
    • G11C11/02Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using magnetic elements
    • G11C11/16Digital stores characterised by the use of particular electric or magnetic storage elements; Storage elements therefor using magnetic elements using elements in which the storage effect is based on magnetic spin effect
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F10/00Thin magnetic films, e.g. of one-domain structure
    • H01F10/32Spin-exchange-coupled multilayers, e.g. nanostructured superlattices
    • H01F10/324Exchange coupling of magnetic film pairs via a very thin non-magnetic spacer, e.g. by exchange with conduction electrons of the spacer
    • H01F10/3254Exchange coupling of magnetic film pairs via a very thin non-magnetic spacer, e.g. by exchange with conduction electrons of the spacer the spacer being semiconducting or insulating, e.g. for spin tunnel junction [STJ]
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F10/00Thin magnetic films, e.g. of one-domain structure
    • H01F10/32Spin-exchange-coupled multilayers, e.g. nanostructured superlattices
    • H01F10/324Exchange coupling of magnetic film pairs via a very thin non-magnetic spacer, e.g. by exchange with conduction electrons of the spacer
    • H01F10/3295Spin-exchange coupled multilayers wherein the magnetic pinned or free layers are laminated without anti-parallel coupling within the pinned and free layers
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F41/00Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
    • H01F41/14Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for applying magnetic films to substrates
    • H01F41/30Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for applying magnetic films to substrates for applying nanostructures, e.g. by molecular beam epitaxy [MBE]
    • H01F41/302Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for applying magnetic films to substrates for applying nanostructures, e.g. by molecular beam epitaxy [MBE] for applying spin-exchange-coupled multilayers, e.g. nanostructured superlattices
    • H01F41/305Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for applying magnetic films to substrates for applying nanostructures, e.g. by molecular beam epitaxy [MBE] for applying spin-exchange-coupled multilayers, e.g. nanostructured superlattices applying the spacer or adjusting its interface, e.g. in order to enable particular effect different from exchange coupling
    • H01F41/307Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for applying magnetic films to substrates for applying nanostructures, e.g. by molecular beam epitaxy [MBE] for applying spin-exchange-coupled multilayers, e.g. nanostructured superlattices applying the spacer or adjusting its interface, e.g. in order to enable particular effect different from exchange coupling insulating or semiconductive spacer
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N50/00Galvanomagnetic devices
    • H10N50/01Manufacture or treatment
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N50/00Galvanomagnetic devices
    • H10N50/10Magnetoresistive devices
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F10/00Thin magnetic films, e.g. of one-domain structure
    • H01F10/32Spin-exchange-coupled multilayers, e.g. nanostructured superlattices
    • H01F10/324Exchange coupling of magnetic film pairs via a very thin non-magnetic spacer, e.g. by exchange with conduction electrons of the spacer
    • H01F10/3268Exchange coupling of magnetic film pairs via a very thin non-magnetic spacer, e.g. by exchange with conduction electrons of the spacer the exchange coupling being asymmetric, e.g. by use of additional pinning, by using antiferromagnetic or ferromagnetic coupling interface, i.e. so-called spin-valve [SV] structure, e.g. NiFe/Cu/NiFe/FeMn
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10BELECTRONIC MEMORY DEVICES
    • H10B61/00Magnetic memory devices, e.g. magnetoresistive RAM [MRAM] devices
    • H10B61/20Magnetic memory devices, e.g. magnetoresistive RAM [MRAM] devices comprising components having three or more electrodes, e.g. transistors
    • H10B61/22Magnetic memory devices, e.g. magnetoresistive RAM [MRAM] devices comprising components having three or more electrodes, e.g. transistors of the field-effect transistor [FET] type

Definitions

  • Magnetoresistive element method for manufacturing magnetoresistive element, and magnetic random access memory
  • the present invention relates to a magnetoresistive effect element, a magnetoresistive effect element manufacturing method, and a magnetic random access memory, and more particularly to a magnetoresistive effect element using a magnetic tunnel junction and a magnetoresistive effect element manufacturing method, and a magnetic random access memory.
  • a magnetoresistive effect element using a magnetic tunnel junction and a magnetoresistive effect element manufacturing method, and a magnetic random access memory.
  • a magnetic tunnel junction composed of two ferromagnetic layers (a pinned ferromagnetic layer and a free ferromagnetic layer) and a tunnel barrier layer (tunnel insulating layer) sandwiched between these ferromagnetic layers : Magnetic Tunneling Junction).
  • the resistance of a magnetic tunnel junction varies greatly depending on the relative direction of magnetization of the ferromagnetic layer. Such a phenomenon is called a tunneling magneto-resistance effect (TMR effect).
  • TMR effect tunneling magneto-resistance effect
  • the MRAM is configured by arranging memory cells each including an MTJ in a matrix. Magnetization of the pinned ferromagnetic layer as one of the two ferromagnetic layers included in MTJ is fixed, and the magnetization of the free ferromagnetic layer as the other ferromagnetic layer can be reversed. Provided. Data is stored as the direction of the magnetic field of the free ferromagnetic layer. Data is written by passing a current in the vicinity of the magnetic tunnel junction and inverting the magnetic field of the free ferromagnetic layer by the magnetic field generated by the current. Data is read out by detecting the direction of the magnetic layer of the free ferromagnetic layer using the TMR effect.
  • the nail coupling magnetic field cannot be made completely zero. That is, the offset magnetic field can be zeroed by this method.
  • the nail coupling magnetic field has a finite value.
  • the cancellation is performed by the leakage magnetic field of the fixed ferromagnetic layer force or the nail coupling magnetic field of the surface force under the fixed ferromagnetic layer. In such a case, it becomes difficult to suppress variations in characteristics because the number of parameters to be controlled increases other than the nail coupling magnetic field.
  • a technique capable of improving the quality of the tunnel barrier layer is desired.
  • a technology that can make the nail coupling magnetic field zero is desired.
  • a technique capable of improving the characteristics of the magnetoresistive element is desired.
  • a technology that can improve the manufacturing yield is desired.
  • JP-A-2002-158381 discloses a ferromagnetic tunnel junction device and a method for manufacturing the same.
  • this ferromagnetic tunnel junction device an insulating layer or an amorphous magnetic layer is sandwiched between an antiferromagnetic layer containing Mn and the first and twenty-second ferromagnetic layers formed on the antiferromagnetic layer.
  • a magnetic pinned layer having an elliptical structure, a tunnel barrier layer formed on the magnetic pinned layer, and a magnetic free layer formed on the tunnel barrier layer.
  • the insulating layer or amorphous magnetic layer of the magnetic pinned layer may have a function of preventing diffusion of Mn contained in the antiferromagnetic layer.
  • the first ferromagnetic layer of the magnetization pinned layer may be exposed to an oxidizing atmosphere, a nitriding atmosphere, or a carbonizing atmosphere to form an insulating layer of the magnetic pinned film.
  • Japanese Patent Application Laid-Open No. 11-54814 discloses a method for manufacturing a ferromagnetic tunnel junction device.
  • This method for manufacturing a ferromagnetic tunnel junction device is a method for manufacturing a ferromagnetic tunnel junction device having a structure in which a tunnel barrier layer is sandwiched between a first ferromagnetic layer and a second ferromagnetic layer.
  • the method includes forming a tunnel barrier layer by forming a conductive layer having a metal or semiconductor power and then introducing oxygen into a vacuum and oxidizing the surface of the conductive layer with a natural acid.
  • After forming the first ferromagnetic layer it may include a step of introducing oxygen into vacuum to oxidize the surface of the first ferromagnetic layer.
  • Japanese Patent Application Laid-Open No. 2000-196165 discloses a magnetic tunnel element and a method for manufacturing the same.
  • This magnetic tunnel junction device manufacturing method includes a metal, an alloy, an intermetallic compound, an oxide, or a nitrogen containing at least one selected from the group consisting of Fe, Ni, and Co.
  • Japanese Patent Application Laid-Open No. 2004-119903 discloses a magnetoresistive effect element and a method for manufacturing the same.
  • This magnetoresistive element manufacturing method includes (A) a step of forming an antiferromagnetic layer on the upper surface side of a substrate in a vacuum container, and (B) after forming the antiferromagnetic layer, in the vacuum container. Introducing an oxidizing gas (e.g., oxygen gas), (C) exhausting the acidic gas from the vacuum vessel, and (D) exhausting the acidic gas, Forming a fixed ferromagnetic layer on the ferromagnetic layer; (E) forming a tunnel barrier layer on the first ferromagnetic layer; and (F) on the tunnel barrier layer.
  • an oxidizing gas e.g., oxygen gas
  • the magnetoresistive element manufacturing method includes (G) a step of forming an antiferromagnetic layer on the upper surface side of the substrate and (H) an antiferromagnetic layer in an atmosphere containing an oxidizing gas (eg, oxygen gas). Forming a fixed ferromagnetic layer on the layer; (I) forming a tunnel barrier layer on the fixed ferromagnetic layer; and ⁇ forming a free ferromagnetic layer on the tunnel barrier layer. Including the step of. The partial pressure of the acidic gas during the step (ii) is determined so that the formed first ferromagnetic layer has conductivity.
  • an oxidizing gas eg, oxygen gas
  • Japanese Patent Application Laid-Open No. 2000-150984 discloses a technique of a magnetic tunnel element using an ozone oxidation insulating film.
  • the magnetic tunnel element using the ozonate insulating film is a magnetic tunnel element having a hard magnetic film and a soft magnetic film having mutually different coercive forces, and an insulating film interposed between the two.
  • the film is oxidized in a mixture of oxygen and ozone.
  • Japanese Unexamined Patent Application Publication No. 2003-258335 discloses a method for manufacturing a tunnel magnetoresistive effect element. This is because the first ferromagnetic layer, the tunnel insulating layer, and the second ferromagnetic layer are laminated in this order on the substrate, and the relative angle difference between the first ferromagnetic layer and the second ferromagnetic layer in the magnetic field direction is different. This is a method of manufacturing a tunnel magnetoresistive element having different tunnel magnetoresistance. A first step of forming a conductive layer as the tunnel insulating layer precursor; and a second step of oxidizing the conductive layer in an oxygen atmosphere.
  • the conductive layer is 0.4 on Dustrom At least one kind of Al, Mg, Si, Ta is formed at a deposition rate of Z seconds or less.
  • the tunnel insulating layer may be formed by performing the first step and the second step a plurality of times.
  • An oxidation method that can be oxidized in vacuum in the second step may be a natural oxidation method, a plasma oxidation method, or a radical oxidation method.
  • an object of the present invention is to provide a magnetoresistive element capable of improving the quality of a tunnel barrier layer in a magnetic tunnel junction, a method for manufacturing the magnetoresistive element, and a magnetic random access memory. It is in.
  • Another object of the present invention is to provide a magnetoresistive effect element, a magnetoresistive effect element manufacturing method, and a magnetoresistive random access memory capable of making a nail coupling magnetic field in a magnetic tunnel junction zero. There is.
  • Still another object of the present invention is to provide a magnetoresistive effect element capable of improving the characteristics of the magnetic tunnel junction, a method for manufacturing the magnetoresistive effect element, and a magnetic random access memory.
  • Another object of the present invention is to provide a magnetoresistive effect element capable of improving the manufacturing yield, a magnetoresistive effect element manufacturing method, and a magnetic random access memory.
  • the method of manufacturing a magnetoresistive element includes forming an antiferromagnetic layer on the upper surface side of the substrate, and forming a first fixed ferromagnetic layer on the antiferromagnetic layer on the upper surface side of the substrate. Forming a layer, exposing the first pinned ferromagnetic layer to a gas containing oxygen atoms at a pressure of 5 X 10 _7 Pa or more and 1 X 10 _4 Pa or less, and Forming a second pinned ferromagnetic layer on the first layer, forming a tunnel barrier layer on the second pinned ferromagnetic layer, and forming a free ferromagnetic layer on the tunnel barrier layer.
  • the gas containing oxygen atoms is exemplified by oxygen gas having a pressure (or partial pressure) of 5 ⁇ 10 _7 Pa or more and 1 ⁇ 10 _4 Pa or less.
  • the second pinned ferromagnetic layer is formed so that the film thickness is greater than 0 and less than or equal to 1 nm.
  • a method for manufacturing a magnetoresistive effect element includes: forming an antiferromagnetic layer on an upper surface side of a substrate; and a first fixed ferromagnetic layer on the antiferromagnetic layer. Forming And exposing the first pinned ferromagnetic layer to a gas containing oxygen atoms at a pressure of 5 X 10 _7 Pa or more and less than 1 X 10 _4 Pa, and a tunnel barrier layer on the first pinned ferromagnetic layer. And forming a free ferromagnetic layer on the tunnel barrier layer.
  • a gas containing oxygen atoms is exemplified by an oxygen gas having a pressure (or partial pressure) of 5 ⁇ 10 _7 Pa or more and less than 1 ⁇ 10 _4 Pa.
  • the step of exposing the first pinned ferromagnetic layer to a gas containing oxygen atoms is performed at a pressure of 1 X 10 _6 Pa or more and 1 X 10 _5 Pa or less. It is more desirable to expose to gases containing oxygen atoms.
  • the gas containing oxygen atoms is preferably a gas containing at least one of oxygen gas, water, methanol, and ethanol gas.
  • the first pinned ferromagnetic layer force includes a film containing one of CoFe, NiFe, CoFeB, and CoFeCr.
  • the surface roughness of the first pinned ferromagnetic layer on the tunnel barrier layer side is smaller than the surface roughness of the lower layer than the first pinned ferromagnetic layer.
  • the magnetoresistive effect element includes an antiferromagnetic layer, a first pinned ferromagnetic layer, a second pinned ferromagnetic layer, a tunnel barrier layer, and a free ferromagnetic layer. It comprises.
  • the antiferromagnetic layer is formed on the upper surface side of the substrate.
  • the first pinned ferromagnetic layer is formed on the antiferromagnetic layer.
  • the second pinned ferromagnetic layer is formed on the first pinned ferromagnetic layer.
  • the tunnel barrier layer is formed on the second pinned ferromagnetic layer.
  • the free ferromagnetic layer is formed on the tunnel barrier layer.
  • the region of the surface of the first pinned ferromagnetic layer on the second pinned ferromagnetic layer side has a higher oxygen concentration than the other regions.
  • the surface roughness of the first pinned ferromagnetic layer on the tunnel barrier layer side is smaller than the surface roughness of the layer below the first pinned ferromagnetic layer.
  • the first pinned ferromagnetic layer includes a pinned ferromagnetic layer A, a nonmagnetic layer, and a pinned ferromagnetic layer B, and is pinned with the pinned ferromagnetic layer A by antiferromagnetic layer coupling via the nonmagnetic layer.
  • the direction of the magnetic field of the ferromagnetic layer B6 is antiparallel.
  • the thickness of the second pinned ferromagnetic layer is greater than 0 and less than or equal to 1 nm.
  • the magnetoresistive effect element includes an antiferromagnetic layer, a first pinned ferromagnetic layer, a tunnel barrier layer, and a free ferromagnetic layer.
  • the antiferromagnetic layer is formed on the upper surface side of the substrate.
  • the first pinned ferromagnetic layer is formed on the antiferromagnetic layer. .
  • the tunnel barrier layer is formed on the first pinned ferromagnetic layer.
  • the free ferromagnetic layer is formed on the tunnel barrier layer.
  • the surface roughness of the first pinned ferromagnetic layer on the tunnel barrier layer side is smaller than the surface roughness of the layer below the first pinned ferromagnetic layer.
  • the magnetoresistive element includes a film containing one of the first fixed ferromagnetic layer forces CoFe, NiFe, CoFeB, and CoFeCr.
  • a magnetic random access memory in another aspect of the present invention, includes a plurality of word lines, a plurality of bit lines, and a plurality of magnetoresistive elements.
  • the plurality of word lines extend in the first direction (X direction).
  • the plurality of bit lines extend in a second direction (Y direction) substantially perpendicular to the first direction (X direction).
  • the plurality of magnetoresistive elements are provided at each of the intersections of the plurality of word lines and the plurality of bit lines, and are described in any one of the above items.
  • FIG. 1 is a cross-sectional view showing a configuration of a first embodiment of a magnetoresistive element of the present invention.
  • FIG. 2 is a cross-sectional view showing a first embodiment of a method for producing a magnetoresistive element of the present invention.
  • FIG. 3 is a cross-sectional view showing a first embodiment of a method for producing a magnetoresistive element of the present invention.
  • FIG. 4 is a cross-sectional view showing a first embodiment of a method for producing a magnetoresistive element of the present invention.
  • FIG. 5 is a cross-sectional view showing a first embodiment of a method for producing a magnetoresistive element of the present invention.
  • FIG. 6 is a cross-sectional view showing a first embodiment of a method for producing a magnetoresistive element of the present invention.
  • FIG. 7 is a graph showing the relationship between the processing conditions in the oxygen gas processing and the nail coupling magnetic field.
  • FIG. 8 is a cross-sectional view showing a configuration of a second embodiment of the magnetoresistance effect element of the present invention.
  • FIG. 9 is a cross-sectional view showing a second embodiment of the method for producing a magnetoresistive element of the present invention.
  • FIG. 10 is a cross-sectional view showing a second embodiment of the method for manufacturing a magnetoresistive element of the present invention.
  • FIG. 11 is a cross-sectional view showing a second embodiment of the method for producing a magnetoresistive element of the present invention.
  • FIG. 12 is a cross-sectional view showing a second embodiment of the method for producing a magnetoresistive element of the present invention.
  • FIG. 13 is a cross-sectional view showing a second embodiment of the method for manufacturing a magnetoresistive element of the present invention.
  • FIG. 14 is a cross-sectional view showing a second embodiment of the method for producing a magnetoresistive element of the present invention.
  • FIG. 15 is a graph showing the relationship between the processing conditions in the oxygen gas processing and the nail coupling magnetic field.
  • FIG. 16 is a graph showing the rate of change in magnetic field resistance of a magnetoresistive effect element manufactured by using the magnetoresistive effect element manufacturing method.
  • FIG. 17 is a graph showing the bias voltage dependence of the MR ratio between a magnetoresistive effect element manufactured using a magnetoresistive effect element manufacturing method and a magnetoresistive effect element manufactured using a conventional method. .
  • FIG. 18 is a cross-sectional view showing a configuration of a memory cell in which the magnetoresistive element of the present invention is applied to a magnetic random access memory.
  • FIG. 19 is a block diagram showing a configuration of an MRAM using memory cells.
  • FIG. 1 is a cross-sectional view showing the configuration of the first embodiment of the magnetoresistive element of the present invention.
  • the magnetoresistive effect element 30 is provided on the upper surface side of the substrate 20, and includes a seed layer 2, an antiferromagnetic layer 3, a fixed ferromagnetic layer A4, a nonmagnetic film 5, a fixed ferromagnetic layer B6, a tunnel barrier layer 7, A free ferromagnetic layer 8 and a cap layer 9 are provided.
  • the seed layer 2 is connected to the lower electrode 1 on the substrate 20 side, and the cap layer 9 is connected to the upper electrode (not shown) on the opposite side.
  • the substrate 20 is a substrate in which an element exemplified by CMOS (for MRAM) is formed on a semiconductor substrate.
  • the lower electrode 1 is provided on the upper surface side of the substrate 20.
  • a conductive material such as Ta, TaN, Rh, Ir is used.
  • the seed layer 2 is provided on the lower electrode 1.
  • a material such as NiFe, CoFe, NiCr, or NiFeCr is used.
  • the antiferromagnetic layer 3 is provided on the seed layer 2.
  • an antiferromagnetic material such as IrMn, FeMn, PtMn, Ni02, or a-Fe203 is used.
  • the fixed ferromagnetic layer A4 is provided on the antiferromagnetic layer 3.
  • a ferromagnetic material such as CoFe, NiFe, CoFeB, or CoFeCr is used.
  • the nonmagnetic layer 5 is provided on the pinned ferromagnetic layer A4.
  • a nonmagnetic material such as Ru or Cu is used.
  • the fixed ferromagnetic layer B6 is provided on the nonmagnetic layer 5.
  • the fixed ferromagnetic layer B6 for example, a ferromagnetic material such as CoFe, NiFe, CoFeB, and CoFeCr is used.
  • an oxygen group is adsorbed on the surface of the fixed ferromagnetic layer B6 by introducing a gas containing oxygen atoms into a vacuum at a predetermined pressure and exposing the surface thereof.
  • a gas containing oxygen atoms oxygen gas, methanol, water, ethanol and the like are used.
  • the tunnel barrier layer 7 is provided on the fixed ferromagnetic layer B6.
  • the tunnel barrier layer 7 is an insulating nonmagnetic material formed by, for example, oxidizing A1 using oxygen radicals, oxygen plasma, ozone, or the like.
  • the free ferromagnetic layer 8 is composed of the tunnel barrier layer 7 It is provided above.
  • the cap layer 9 is provided on the free ferromagnetic layer 8.
  • a conductive material such as Ta, TaN, Rh, Ir is used.
  • the unevenness of each film shows general unevenness that is not intentional and can be naturally formed during film formation.
  • the tunnel barrier layer 7 is a smooth layer with reduced irregularities on the surface of the free ferromagnetic layer 8 side. Along with this, the layers above it have also become smooth.
  • 2 to 6 are sectional views showing a method of manufacturing a magnetoresistive effect element according to the first embodiment of the present invention.
  • lower electrode 1, seed layer 2, antiferromagnetic layer 3, pinned ferromagnetic layer A4, nonmagnetic layer 5, and pinned ferromagnetic layer B6 are formed in this order on the upper surface of substrate 1. Is done. Film formation is performed using a notched method, an ion beam sputtering method, or the like.
  • the surface of the fixed ferromagnetic layer B6 is exposed to oxygen gas. Adsorb oxygen on the surface.
  • the pressure (partial pressure) of the oxygen gas is made very small. Thereby, the surface of the pinned ferromagnetic layer B6 has only oxygen adsorbed or has an extremely thin layer containing a large amount of oxygen, and there is no oxide layer of the pinned ferromagnetic layer B6.
  • It may be a substance containing an OH group such as methanol, water, and ethanol, or a gas combining two or more of oxygen gas, methanol, water, and ethanol.
  • tunnel barrier film 7a is formed on fixed ferromagnetic layer B6 after the surface treatment. Film formation is performed using a sputtering method, an ion beam sputtering method, or the like. As described above, the tunnel barrier film 7a is a continuous film without pinholes even if it is thin. At this time, the surface roughness of the film (average surface roughness Ra, maximum surface roughness Rmax) decreases, and the unevenness is reduced. There will be no film. At the same time, the period of the surface roughness does not follow the undulation of the surface of the lower layer such as the fixed ferromagnetic layer B6, and the undulation period becomes shorter.
  • tunnel barrier layer film 7a is oxidized using oxygen plasma. Instead of oxygen plasma, oxygen radicals or ozone may be used for oxidation. As a result, the tunnel barrier layer film 7 a is oxidized and becomes an insulating tunnel barrier layer 7.
  • the tunnel barrier layer 7 is a thin, continuous layer without pinholes.
  • a free ferromagnetic layer 8 and a cap layer 9 are formed in this order on the tunnel barrier layer 7. Thereafter, an upper electrode (not shown) is formed.
  • FIG. 2 the manufacturing method of the magnetoresistive effect element is performed.
  • FIG. 4-6 the method of FIG. 2, FIG. 4-6 can also use the other method well-known to those skilled in the art.
  • FIG. 7 is a graph showing the relationship between the processing conditions in the oxygen gas processing of FIG. 3 and the nail coupling magnetic field.
  • the vertical axis is the magnitude of the nail coupling magnetic field (Oe), and the horizontal axis is the oxygen exposure time (seconds).
  • Each curve in the graph shows a case of different oxygen gas pressure (oxygen gas partial pressure).
  • Oxygen gas pressure, diamonds l X 10 _7 Pa, square l X 10 _6 Pa, triangle 1 X 10 _5 Pa, back is 1 X 10 _4 Pa. As shown in Fig.
  • the oxygen gas pressure is preferably 1 X 10 " 7 Pa or more and less than 1 X 10 _4 Pa.
  • the gas pressure is more preferable in production.
  • the surface of the fixed ferromagnetic layer B6 is in a state where oxygen is adsorbed or an extremely thin layer containing a large amount of oxygen. Can be formed.
  • the wettability of the tunnel barrier layer film 7a to the fixed ferromagnetic layer B6 is improved, and a continuous film can be formed even if it is thin. That is, the growth method of the tunnel barrier layer film 7a can be changed, and the flatness (surface roughness) of the tunnel barrier layer 7 formed by oxidizing the tunnel barrier layer film 7a can be changed. be able to.
  • the magnitude of the nail coupling magnetic field can be reduced to zero.
  • the size can be set to zero.
  • the magnitude of the nail coupling magnetic field can be reduced to zero by adjusting the treatment conditions.
  • the pressure of the gas is set to be the same as the amount of oxygen atoms contained in the oxygen gas having a pressure of 1 X 10 _7 Pa or more and less than 1 X 10 _4 Pa, for example. .
  • the surface force of the tunnel barrier layer 7 on the fixed ferromagnetic layer B6 side and the surface force on the free ferromagnetic layer 8 side are respectively pinned on the tunnel barrier layer 7. It is adjusted to an appropriate surface roughness that does not generate holes. Therefore, according to the present invention, the magnitude of the Neel coupling magnetic field can be reduced to 0 while suppressing the generation of pinholes in the tunnel barrier layer 7.
  • FIG. 8 is a cross-sectional view showing the configuration of the magnetoresistive effect element according to the second exemplary embodiment of the present invention.
  • the magnetoresistive effect element 30a is provided on the upper surface side of the substrate 20, and includes a seed layer 2, an antiferromagnetic layer 3, a fixed ferromagnetic layer A4, a nonmagnetic film 5, a fixed ferromagnetic layer B6, a boundary layer 10, and a fixed layer.
  • the seed layer 2 is connected to the lower electrode 1
  • the cap layer 9 is connected to the upper electrode (not shown).
  • the magnetoresistive effect element 30a of this embodiment is different from that of the first embodiment in that a boundary layer 10 and a fixed ferromagnetic layer CI1 are provided between the fixed ferromagnetic layer B6 and the tunnel barrier layer 7.
  • the boundary layer 10 is formed by introducing a gas containing oxygen atoms into a vacuum at a predetermined pressure to expose the surface of the pinned ferromagnetic layer B6. .
  • the pressure (partial pressure) of the oxygen gas is made very small.
  • the boundary layer 10 has an oxygen adsorption layer on the surface of the pinned ferromagnetic layer B6, or a large amount of oxygen. It is formed as a very thin (including one to two molecules) layer, and there is no oxide layer of the fixed pinned ferromagnetic layer B6.
  • the gas containing oxygen atoms oxygen gas, methanol, water, ethanol and the like are used.
  • the fixed ferromagnetic layer C11 is provided on the boundary layer 10. Ferromagnetic materials such as CoFe, NiFe, CoFeB, and CoFeCr are used for the fixed ferromagnetic layer C11. Before forming the tunnel barrier layer 7, an oxygen group may be adsorbed on the surface by introducing a gas containing oxygen atoms into a vacuum at a predetermined pressure to expose the surface of the fixed ferromagnetic layer C11. As gas containing oxygen atoms, oxygen gas, methanol, water, ethanol, etc. are used.
  • the unevenness of each film indicates general unevenness that is not intentional and can be naturally formed during film formation.
  • the pinned ferromagnetic layer C11 has a smooth surface with reduced surface irregularities on the free ferromagnetic layer 8 side. Along with this, the layers above it are also smooth.
  • 9 to 14 are cross-sectional views showing a method of manufacturing a magnetoresistive effect element according to the second embodiment of the present invention.
  • lower electrode 1, seed layer 2, antiferromagnetic layer 3, pinned ferromagnetic layer A4, nonmagnetic layer 5, and pinned ferromagnetic layer B6 are formed in this order on the upper surface of substrate 1. Is done. Film formation is performed using a notched method, an ion beam sputtering method, or the like.
  • the surface of fixed ferromagnetic layer B6 is exposed to oxygen gas by introducing oxygen gas (or a gas containing oxygen gas at the same partial pressure) into a vacuum.
  • oxygen gas or a gas containing oxygen gas at the same partial pressure
  • the boundary layer 10 is formed on the surface of the pinned ferromagnetic layer B6.
  • the boundary layer 10 is an oxygen adsorption layer on the surface of the fixed ferromagnetic layer B6 or an extremely thin layer containing a large amount of oxygen.
  • a substance containing an OH group such as methanol, water, ethanol, or a gas combining two or more of oxygen gas, methanol, water, and ethanol may be used.
  • the pinned ferromagnetic layer C11 grows by surface force of the boundary layer 10, so that the boundary layer 10 of the pinned ferromagnetic layer C11 (pinned ferromagnetic layer) B6) Improves. Also, the crystalline state is different from that formed directly on the pinned ferromagnetic layer B6.
  • the fixed ferromagnetic layer C11 is formed on the boundary layer 10.
  • Film formation is performed using a sputtering method, an ion beam sputtering method, or the like.
  • the surface state of the boundary layer 10 is different from that of the normal pinned ferromagnetic layer B6, the surface state force of the formed pinned ferromagnetic layer C11 is different from that of the normal pinned ferromagnetic layer B6. Will be different.
  • the surface roughness (average surface roughness Ra, maximum surface roughness Rmax) of the film decreases, and the film has less unevenness.
  • the period of the surface roughness does not follow the surface waviness of the lower layer (such as the fixed ferromagnetic layer B6), and the waviness period becomes shorter.
  • the tunnel barrier layer film 7a is formed, the wettability of the tunnel barrier layer film 7a with respect to the fixed ferromagnetic layer C11 is improved, and the film can be made continuous even without being thin and without pinholes. It becomes possible.
  • tunnel barrier layer film 7a is formed on fixed ferromagnetic layer C11. Film formation is performed using a sputtering method, an ion beam sputtering method, or the like. As described above, the tunnel barrier layer film 7a is a continuous film that does not have pinholes even if it is thin. Referring to FIG. 13, tunnel barrier film 7a is oxidized using oxygen plasma. Instead of oxygen plasma, oxygen radicals or ozone may be used for oxidation. Accordingly, the tunnel noria film 7a is oxidized to become an insulating tunnel barrier layer 7. The tunnel barrier layer 7 is a thin layer without a continuous pinhole.
  • a free ferromagnetic layer 8 and a cap layer 9 are formed in this order on the tunnel barrier layer 7. Thereafter, an upper electrode (not shown) is formed.
  • FIG. 9, FIG. 12-FIG. 14 can also use the other method well-known to those skilled in the art. In this manufacturing method, the same effect can be obtained by forming the remaining pinned ferromagnetic layer C11 in FIG. 11 in a gas atmosphere containing oxygen atoms.
  • FIG. 15 is a graph showing the relationship between processing conditions and the nail coupling magnetic field in the oxygen gas processing of FIG.
  • the vertical axis is the magnitude of the nail coupling magnetic field (Oe), and the horizontal axis is the film thickness (nm) of the fixed ferromagnetic layer C11.
  • Each curve in the graph shows the case of different oxygen gas pressure (oxygen gas partial pressure).
  • Oxygen gas pressure is l X 10 _7 Pa for diamond and 1 X 1 for square 0 _b Pa, the triangle is 1 X 10 _4 Pa, and the back is 1 X 10 _d Pa.
  • the oxygen exposure time is 240 seconds.
  • the oxygen gas pressure is between 1 X 10 _7 Pa and less than 1 X 10 _3 Pa. It can be seen that there is a condition where the nail coupling magnetic field is zero when in the very low pressure range. That is, the oxygen gas pressure is preferably 1 ⁇ 10 _7 Pa or more and 1 ⁇ 10 _4 Pa or less. However, a gas pressure of 1 ⁇ 10_6 Pa or more and 1 ⁇ 10_5 Pa or less is preferable from the viewpoint of adjustment of oxygen gas pressure. When the film thickness of the fixed layer ferromagnetic layer C11 is greater than lnm, the nail coupling magnetic field is zero.
  • the oxygen adsorption layer on the surface of the fixed ferromagnetic layer B6 or the acid layer of the extremely thin fixed ferromagnetic layer B6 is changed by changing the pressure of the oxygen gas in the oxygen atmosphere to be exposed. It is possible to form the boundary layer 10 which is a soot layer. Further, by changing the surface state of the pinned ferromagnetic layer B6 at the boundary layer 10, the crystal state of the pinned ferromagnetic layer C11 can be changed. Since the surface state of the pinned ferromagnetic layer C11 changes, when the tunnel barrier layer film 7a is formed, the tunnel barrier layer film 7a has a surface force on the pinned ferromagnetic layer C11. Film can be formed.
  • the growth method of the tunnel barrier layer film 7a can be changed, and the flatness of the upper surface of the tunnel barrier layer 7 formed by oxidizing the tunnel barrier layer film 7a can be changed. .
  • the magnitude of the nail coupling magnetic field can be reduced to zero.
  • the magnitude of the nail coupling magnetic field can be reduced to zero by adjusting the conditions for treating oxygen gas.
  • nail coupling can be achieved by adjusting the processing conditions. It is possible to reduce the magnitude of the magnetic field to zero.
  • the oxygen gas treatment of the surface of the fixed ferromagnetic layer B 6 by the oxygen gas treatment of the surface of the fixed ferromagnetic layer B 6, the surface force of the tunnel barrier layer 7 on the fixed ferromagnetic layer B 6 side and the surface force of the free ferromagnetic layer 8 side are respectively pinned on the tunnel barrier layer 7. It is adjusted to an appropriate surface roughness that does not generate holes. Therefore, according to the present invention, while preventing the generation of pinholes in the tunnel barrier layer 7, The magnitude of the magnetic field can be reduced to zero.
  • the material of the pinned ferromagnetic layer B6 is changed, the optimum oxygen exposure conditions differ depending on changes in the wettability of oxygen gas. Good wettability! ⁇ Materials have a shorter oxygen exposure time and poor wettability, and materials have a longer oxygen exposure time.
  • FIG. 16 is a graph showing the rate of change in magnetic field resistance of the magnetoresistive effect element in the magnetic tunnel junction manufactured by using the above manufacturing method (first example or second example).
  • the vertical axis is the magnetoresistance (MR) change rate (%) of the magnetoresistive effect element (MTJ film), and the horizontal axis is the magnitude (Oe) of the magnetic field applied to the magnetoresistive effect element. Due to the effect of the smoothing of the tunnel barrier layer 7, a resistance change rate of about 40% was obtained at a bias voltage of lOOmV.
  • FIG. 17 shows a magnetoresistive effect element (MTJ film) (a) manufactured using the above manufacturing method (first embodiment or second embodiment) (a) and a magnetoresistive effect element (MTJ film) manufactured by a conventional method. It is a graph which shows the bias voltage dependence of MR ratio (resistance change rate (%)) with (b).
  • the magnetoresistive effect element manufactured using the present invention has a higher MR ratio than the conventional magnetoresistive effect element at any bias voltage. This is a result of the improved quality of the tunnel barrier layer 7 (alumina). In other words, the quality of the tunnel barrier layer in the magnetic tunnel junction of the magnetoresistive effect element can be improved, the nail coupling magnetic field can be made zero, and the characteristics of the magnetic tunnel junction of the magnetoresistive effect element can be improved. It becomes.
  • FIG. 18 is a cross-sectional view showing the configuration of a memory cell in which the magnetoresistive element of the present invention is applied to a magnetic random access memory.
  • the memory cell 42 includes the magnetoresistive effect element 30 (or 30a), the lower electrode 1, the upper electrode 31, the MOS transistor 46, the contact wiring 47, and the contact wiring 48 described above.
  • the memory cell 42 is connected to the write word line 43, the read word line 44, the bit line 45, and the GND line 50.
  • the MOS transistor 46 includes a first diffusion layer 46a and a second diffusion layer provided in the semiconductor substrate. 46c, and a first gate 46b provided on the semiconductor substrate between the first diffusion layer 46a and the second diffusion layer 46c via an insulating layer.
  • the first diffusion layer 46 a is connected to the GND line 50 via the contact wiring 48.
  • the second diffusion layer 46 c is connected to one end of the lower electrode 1 through the contact wiring 47.
  • the gate 46b is connected to the read word line 44.
  • the lower electrode 1 is connected to one end side of the magnetoresistive effect element 30 (30a) at the other end.
  • the magnetoresistive effect element 30 (30a) is the magnetoresistive effect element (magnetic tunnel junction element) described in the first embodiment or the second embodiment.
  • the magnetoresistive effect element 30 (30a) is connected to the bit line 45 via the upper electrode 31 on the other end side.
  • a write word line 43 is provided on the opposite side to the bit line 45 with respect to the magnetoresistive effect element 30 (30a) via the lower electrode 1 and the interlayer insulating layer 49 so as to be orthogonal to the bit line 45. ing.
  • the spontaneous magnetization of the free ferromagnetic layer 8 includes the current flowing through the bit line 45 passing over the memory cell 42 and the write word passing under the memory cell 42. It is reversed in the desired orientation by the resultant magnetic field induced by the current flowing in line 43.
  • FIG. 19 is a block diagram showing a configuration of the MRAM 60 using the memory cell 42.
  • the MRAM 60 includes a plurality of memory cells 42, a plurality of reference memory cells 42r, a plurality of write word lines 43, a plurality of read word lines 44, a plurality of bit lines 45, an X selector 58, and an X-side current source circuit. 59, an X side current termination circuit 56, a Y selector 51, a Y side current source circuit 52, a read current load circuit 53, a Y side current termination circuit 54, and a sense amplifier 55.
  • the memory cells 42 are provided corresponding to the intersections of the plurality of write word lines 43 (the plurality of read word lines 44) and the plurality of bit lines 45, and are arranged in a matrix.
  • the X selector 58 writes a desired selected read word line 44 s during a read operation from a plurality of read word lines 44 and a plurality of write word lines 43 extending in the X-axis direction (word line direction). Sometimes the desired selective write word line 43s is selected.
  • the X-side current source circuit 59 is a constant current source that supplies a constant current during a data write operation to the memory cell 42.
  • the X-side current termination circuit 56 terminates the plurality of write word lines 43.
  • the Y selector 51 selects a desired selected bit line 45s from the plurality of bit lines 45 extending in the Y-axis direction (bit line direction).
  • the Y-side current source circuit 52 is a constant current source that supplies a constant current during a data write operation to the memory cell 42.
  • Read current load circuit 53 This is a constant current source that supplies a predetermined current to the selected memory cell 42 (hereinafter, selected cell 42 s) and the reference memory cell 42 r during the data read operation from the memory cell 42.
  • the Y side current termination circuit 54 terminates the plurality of bit lines 45.
  • the sense amplifier 55 outputs the data of the selected cell 42s based on the difference between the voltage of the reference bit line 45r connected to the memory cell 42r for reference and the voltage of the bit line 45 connected to the selected cell 42s.
  • Reading data from the memory cell 42 is performed as follows. That is, for the magnetoresistive effect element 30 (30a) of the selected cell 42s corresponding to the intersection of the selected read word line 44s selected by the X selector 58 and the selected bit line 45s selected by the Y selector 51 Thus, a constant current is supplied by the read current load circuit 53. As a result, the selected bit line 45 s has a voltage corresponding to the state of the free ferromagnetic layer 8 of the magnetoresistive element 30 (30a) (the resistance value of the magnetoresistive element 30 (30a)). It becomes.
  • a constant current is similarly supplied to the reference memory cell 42r selected by the bit line 45r and the selected read word line 44s, and the bit line 45r has a predetermined reference voltage. Then, the sense amplifier 55 compares the magnitudes of the two voltages. For example, if the voltage of the selected bit line 45s is greater than the reference voltage, the data of the selected cell 42s is determined to be “1”, and if it is smaller, “0”.
  • Data is written to the memory cell 42 as follows. That is, for the magnetoresistive effect element 30 (30a) of the selected cell 42s corresponding to the intersection of the selected write word line 43s selected by the X selector 58 and the selected bit line 45s selected by the Y selector 51, A magnetic field H in the Y direction and a magnetic field H in the X direction are generated. As a result, a composite magnetic field H is generated.
  • the magnetic field H is applied to the selective write word line 43s by the X-side current source circuit 59.
  • the magnetic field H is applied to the Y-side current source on the selected bit line 45s.
  • the magnetoresistive effect element 30 (30a) receives the combined magnetic field H and reverses the direction of spontaneous magnetization so as to correspond to the data to be written.
  • the magnetoresistive effect element of the first and second embodiments By using the magnetoresistive effect element of the first and second embodiments, the quality of the tunnel barrier layer in the magnetic tunnel junction of the magnetoresistive effect element is improved, and the nail coupling magnetic field is made zero. Can improve the characteristics of the magnetic tunnel junction of the magnetoresistive effect element It becomes possible to do. By using this magnetoresistive element for a magnetic random access memory, it becomes possible to improve the manufacturing yield of the magnetic random access memory.
  • the upper and lower surfaces of the tunnel barrier layer can be made smooth, the quality of the tunnel barrier layer can be improved, and a high MR MRAM can be manufactured.
  • the offset magnetic field can be easily adjusted to zero by setting the nail coupling magnetic field to zero. As a result, it is possible to manufacture an MRAM in which the write current that is strong against the disturbance between the memory cells 42 is kept low.
  • the magnetoresistance effect element of the present invention can also be used in a magnetic head of a magnetic disk device.
  • the nail coupling magnetic field in the magnetic tunnel junction can be made zero, and the quality of the tunnel barrier layer can be improved.

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Abstract

A method for manufacturing a magnetoresistive device comprises a step for forming an antiferromagnetic layer on the upper surface of a substrate, a step for forming a first fixed ferromagnetic layer on the antiferromagnetic layer on the upper surface of the substrate, a step for exposing the first fixed ferromagnetic layer to a gas containing oxygen atoms at a pressure of not less than 5 × 10-7 Pa and not more than 1 × 10-4 Pa, a step for forming a second fixed ferromagnetic layer on the first fixed ferromagnetic layer, a step for forming a tunnel barrier layer on the second fixed ferromagnetic layer, and a step for forming a free ferromagnetic layer on the tunnel barrier layer. In this connection, an oxygen gas having a pressure (partial pressure) of not less than 5 × 10-7 Pa and not more than 1 × 10-4 Pa exemplifies the gas containing oxygen atoms. In this method for manufacturing a magnetoresistive device, the second fixed ferromagnetic layer is so formed as to have a thickness of more than 0 and not more than 1 nm.

Description

明 細 書  Specification

磁気抵抗効果素子及び磁気抵抗効果素子の製造方法、磁気ランダムァ クセスメモリ  Magnetoresistive element, method for manufacturing magnetoresistive element, and magnetic random access memory

技術分野  Technical field

[0001] 本発明は、磁気抵抗効果素子及び磁気抵抗効果素子の製造方法、磁気ランダム アクセスメモリに関し、特に磁気トンネル接合を用いる磁気抵抗効果素子及び磁気抵 抗効果素子の製造方法、磁気ランダムアクセスメモリに関する。  The present invention relates to a magnetoresistive effect element, a magnetoresistive effect element manufacturing method, and a magnetic random access memory, and more particularly to a magnetoresistive effect element using a magnetic tunnel junction and a magnetoresistive effect element manufacturing method, and a magnetic random access memory. About.

背景技術  Background art

[0002] 2つの強磁性体層(固定強磁性層及び自由強磁性層)と、これらの強磁性体層に 挟まれたトンネルバリア層(トンネル絶縁層)とで構成される磁気トンネル接合 (MTJ : Magnetic Tunneling Junction)が知られている。磁気トンネル接合は、強磁性 体層の磁化の相対方向に依存して、その抵抗が大きく変化する。このような現象は、 トンネル磁気抵抗効果(TMR効果: Tunneling Magneto - Resistance 効果)と 呼ばれる。磁気トンネル接合の抵抗を検出することにより、強磁性体層の磁化の方向 を判別することが可能である。このような磁気トンネル接合の性質は、磁気トンネル接 合を含む磁気抵抗デバイスとして、不揮発的にデータを保持する磁気ランダムァクセ スメモリ (MRAM: Magnetic Randam Access Memory)に適用される。  [0002] A magnetic tunnel junction (MTJ) composed of two ferromagnetic layers (a pinned ferromagnetic layer and a free ferromagnetic layer) and a tunnel barrier layer (tunnel insulating layer) sandwiched between these ferromagnetic layers : Magnetic Tunneling Junction). The resistance of a magnetic tunnel junction varies greatly depending on the relative direction of magnetization of the ferromagnetic layer. Such a phenomenon is called a tunneling magneto-resistance effect (TMR effect). By detecting the resistance of the magnetic tunnel junction, it is possible to determine the magnetization direction of the ferromagnetic layer. Such a property of the magnetic tunnel junction is applied to a magnetic random access memory (MRAM) that holds data in a nonvolatile manner as a magnetoresistive device including the magnetic tunnel junction.

[0003] MRAMは、それぞれに MTJを含むメモリセルが行列に配置されて構成される。 M TJに含まれる 2つの強磁性体層のうちの一方の強磁性層としての固定強磁性層の磁 化は固定され、他方の強磁性層としての自由強磁性層の磁ィ匕は反転可能に設けら れる。データは、自由強磁性層の磁ィ匕の方向として記憶される。データの書き込みは 、磁気トンネル接合の近傍に電流を流し、その電流が発生する磁界によって自由強 磁性層の磁ィ匕を反転することによって行われる。データの読み出しは、 TMR効果を 利用して自由強磁性層の磁ィ匕の向きを検出することによって行われる。  [0003] The MRAM is configured by arranging memory cells each including an MTJ in a matrix. Magnetization of the pinned ferromagnetic layer as one of the two ferromagnetic layers included in MTJ is fixed, and the magnetization of the free ferromagnetic layer as the other ferromagnetic layer can be reversed. Provided. Data is stored as the direction of the magnetic field of the free ferromagnetic layer. Data is written by passing a current in the vicinity of the magnetic tunnel junction and inverting the magnetic field of the free ferromagnetic layer by the magnetic field generated by the current. Data is read out by detecting the direction of the magnetic layer of the free ferromagnetic layer using the TMR effect.

[0004] 固定強磁性層と自由強磁性層との間には、色々な磁気的な相互作用が働く。その 主なものとしてネールカップリング磁界、漏れ磁界がある。このような磁気的な相互作 用があると、自由強磁性層が並行力 反並行にスイッチングするときの磁界の大きさ と、反並行力 平行な方向にスイッチングするときの磁界の大きさが異なる。これらの 反転磁界の大きさの差はオフセット磁界と呼ばれて 、る。このようなオフセット磁界が 存在すると、メモリセル間のディスターブが大きくなる。その場合、磁化反転不良を引 き起こしやすくなるため製造歩留まりが低下してしまう。そのため、オフセット磁界の大 きさはゼロにする必要がある。 [0004] Various magnetic interactions act between the fixed ferromagnetic layer and the free ferromagnetic layer. The main ones are nail coupling magnetic field and leakage magnetic field. With such magnetic interaction, the magnitude of the magnetic field when the free ferromagnetic layer switches parallel force antiparallel And the magnitude of the magnetic field when switching in the parallel direction is different. The difference between the magnitudes of these reversal fields is called the offset magnetic field. When such an offset magnetic field exists, the disturbance between memory cells becomes large. In that case, it becomes easy to cause a magnetization reversal failure, and thus the manufacturing yield decreases. Therefore, the magnitude of the offset magnetic field needs to be zero.

[0005] オフセット磁界をゼロにする方法として、例えば、 USP6292389号に記載されたよ うに、固定強磁性層の上面と下面が相殺するように設定する方法、 USP6233172 号に記載されたように、ネールカップリング磁界と漏れ磁界とを同じ大きさになるよう にして互いにキャンセルするという方法がある。このような方法を用いることにより、ォ フセット磁界をゼロに調整することができる。  [0005] As a method of making the offset magnetic field zero, for example, as described in USP6292389, a method of setting the upper and lower surfaces of the fixed ferromagnetic layer to cancel each other, as described in USP6233172, a nail cup There is a method of canceling each other by making the ring magnetic field and the leakage magnetic field the same magnitude. By using such a method, the offset magnetic field can be adjusted to zero.

[0006] た し、上記 USP6292389号、 USP6233172号【こ記載の磁気抵抗効果素子【こ おいて、トンネルバリア層の下の膜の表面粗さが粗いと、その上に成膜されるトンネル ノ リア層の膜厚が lnm程度と非常に薄いので、トンネルバリア層を連続に形成するこ とが困難である。そうような場合、トンネルバリア層にリークスポットができ、トンネルバリ ァ層の品質が低下してしまう可能性がある。従って、トンネルバリア層の下面をできる だけ平滑にする必要がある。  [0006] However, the above-mentioned USP6292389, USP6233172 [the magnetoresistive effect element described herein] [In this case, if the surface roughness of the film under the tunnel barrier layer is rough, the tunnel noor is formed thereon. Since the thickness of the layer is as thin as 1 nm, it is difficult to form a tunnel barrier layer continuously. In such a case, a leak spot may be formed in the tunnel barrier layer, and the quality of the tunnel barrier layer may be deteriorated. Therefore, it is necessary to make the lower surface of the tunnel barrier layer as smooth as possible.

[0007] カロえて、上記 USP6292389号、 USP6233172号のような磁気抵抗効果素子で は、ネールカップリング磁界を完全にゼロにはできない。すなわち、オフセット磁界は 、この方法でゼロにすることができる力 ネールカップリング磁界は有限な値をもつ。 上記の文献では、固定強磁性層力 の漏れ磁界、あるいは固定強磁性層の下の面 力 のネールカップリング磁界でキャンセルする。このような場合、ネールカップリング 磁界以外に制御するパラメータが増えるために特性のばらつきを抑えるのが難しくな る。  [0007] With a magnetoresistive element such as USP6292389 and USP6233172, the nail coupling magnetic field cannot be made completely zero. That is, the offset magnetic field can be zeroed by this method. The nail coupling magnetic field has a finite value. In the above document, the cancellation is performed by the leakage magnetic field of the fixed ferromagnetic layer force or the nail coupling magnetic field of the surface force under the fixed ferromagnetic layer. In such a case, it becomes difficult to suppress variations in characteristics because the number of parameters to be controlled increases other than the nail coupling magnetic field.

[0008] トンネルバリア層の下面を平滑にする方法として、 J. Appl. Phys.、 Vol. 93、 No.  [0008] As a method of smoothing the lower surface of the tunnel barrier layer, J. Appl. Phys., Vol. 93, No.

10、 Part2 & 3、 2003、 p. 8373【こ示されるよう【こ、磁気トン才ヽノレ接合を含む磁気抵 抗効果素子を低圧力の DCマグネトロンスパッタで形成することが報告されている。そ れによってネールカップリングの大きさを 2— 30eと 、う低 、値にできると報告されて いる。し力しながら、上記の文献に示される磁気抵抗効果素子では、固定強磁性層 を平滑にした場合、固定強磁性層と反強磁性層の間の交換結合磁界が低下すること が考えられる。一般に反強磁性膜は下地膜の上に結晶成長する。この結晶成長が 進むと交換結合磁界が大きくなる。一方で、結晶成長が進むほど結晶粒の粒に起因 する表面粗さは大きくなる。つまり、交換結合磁界と固定強磁性層の平滑性はトレー ド才フの関係がある。 10, Part 2 & 3, 2003, p. 8373 [As shown, it has been reported that a magnetoresistive element including a magnetic junction is formed by low-pressure DC magnetron sputtering. It has been reported that this can reduce the size of the nail coupling to 2-30e. However, in the magnetoresistive effect element shown in the above document, the fixed ferromagnetic layer It is conceivable that the exchange coupling magnetic field between the pinned ferromagnetic layer and the antiferromagnetic layer is lowered when is smoothed. In general, an antiferromagnetic film grows on a base film. As this crystal growth proceeds, the exchange coupling magnetic field increases. On the other hand, as the crystal growth proceeds, the surface roughness due to the crystal grains increases. In other words, the exchange coupling magnetic field and the smoothness of the fixed ferromagnetic layer have a trade-off relationship.

[0009] トンネルバリア層の品質を向上することが可能な技術が望まれる。ネールカップリン グ磁界をゼロにすることが可能な技術が望まれる。磁気抵抗効果素子の特性を向上 することが可能な技術が望まれる。製造歩留まりを改善することが可能な技術が望ま れる。  [0009] A technique capable of improving the quality of the tunnel barrier layer is desired. A technology that can make the nail coupling magnetic field zero is desired. A technique capable of improving the characteristics of the magnetoresistive element is desired. A technology that can improve the manufacturing yield is desired.

[0010] 上記説明と関連として、特開 2002— 158381号公報に強磁性トンネル接合素子お よびその製造方法が開示されている。この強磁性トンネル接合素子は、 Mnを含有す る反強磁性層と、前記反強磁性層上に形成された、第 1および第 22つの強磁性層 の間に絶縁層またはアモルファス磁性層を挟んだ構造を有する磁ィ匕固着層と、前記 磁化固着層上に形成されたトンネルバリア層と、前記トンネルバリア層上に形成され た磁ィ匕自由層とを具備する。前記磁ィ匕固着層の絶縁層またはアモルファス磁性層が 、前記反強磁性層に含まれる Mnの拡散を防止する機能を有していても良い。前記 磁化固着層の第 1強磁性層を酸化雰囲気、窒化雰囲気または炭化雰囲気に暴露し て、前記磁ィ匕固着膜の絶縁層を形成しても良い。  [0010] In connection with the above description, JP-A-2002-158381 discloses a ferromagnetic tunnel junction device and a method for manufacturing the same. In this ferromagnetic tunnel junction device, an insulating layer or an amorphous magnetic layer is sandwiched between an antiferromagnetic layer containing Mn and the first and twenty-second ferromagnetic layers formed on the antiferromagnetic layer. A magnetic pinned layer having an elliptical structure, a tunnel barrier layer formed on the magnetic pinned layer, and a magnetic free layer formed on the tunnel barrier layer. The insulating layer or amorphous magnetic layer of the magnetic pinned layer may have a function of preventing diffusion of Mn contained in the antiferromagnetic layer. The first ferromagnetic layer of the magnetization pinned layer may be exposed to an oxidizing atmosphere, a nitriding atmosphere, or a carbonizing atmosphere to form an insulating layer of the magnetic pinned film.

[0011] また、特開平 11— 54814号公報に、強磁性トンネル接合素子の製造方法が開示 されている。この強磁性トンネル接合素子の製造方法は、第 1強磁性層と第 2強磁性 層の間にトンネルバリア層を挟んだ構造を持つ強磁性トンネル接合素子の製造方法 である。金属又は半導体力 なる導電層を成膜した後、真空中に酸素を導入し、該 導電層表面を自然酸ィ匕してトンネルバリア層を形成する工程を含む。第 1強磁性層 を成膜した後、真空中に酸素を導入して該第 1強磁性層表面を酸化する工程を含ん でいても良い。  [0011] Also, Japanese Patent Application Laid-Open No. 11-54814 discloses a method for manufacturing a ferromagnetic tunnel junction device. This method for manufacturing a ferromagnetic tunnel junction device is a method for manufacturing a ferromagnetic tunnel junction device having a structure in which a tunnel barrier layer is sandwiched between a first ferromagnetic layer and a second ferromagnetic layer. The method includes forming a tunnel barrier layer by forming a conductive layer having a metal or semiconductor power and then introducing oxygen into a vacuum and oxidizing the surface of the conductive layer with a natural acid. After forming the first ferromagnetic layer, it may include a step of introducing oxygen into vacuum to oxidize the surface of the first ferromagnetic layer.

[0012] また、特開 2000— 196165号公報に、磁気トンネル素子及びその製造方法が開 示されている。この磁気トンネル接合素子の製造方法は、 Fe、 Ni及び Coからなる群 から選択された少なくとも 1種を含有する金属、合金、金属間化合物、酸化物又は窒 化物からなる下磁性層を形成し、前記下磁性層に酸化処理をする工程と、この下磁 性層の上にバリア膜を形成する工程と、前記ノリア膜の上に Fe、 Ni及び Coからなる 群から選択された少なくとも 1種を含有する金属、合金、金属間化合物、酸化物又は 窒化物からなる上磁性層を形成する工程とを有する。 [0012] Japanese Patent Application Laid-Open No. 2000-196165 discloses a magnetic tunnel element and a method for manufacturing the same. This magnetic tunnel junction device manufacturing method includes a metal, an alloy, an intermetallic compound, an oxide, or a nitrogen containing at least one selected from the group consisting of Fe, Ni, and Co. Forming a lower magnetic layer made of an oxide, oxidizing the lower magnetic layer, forming a barrier film on the lower magnetic layer, and forming Fe, Ni and Co on the noria film. Forming an upper magnetic layer made of a metal, an alloy, an intermetallic compound, an oxide or a nitride containing at least one selected from the group consisting of:

[0013] また、特開 2004— 119903号公報に、磁気抵抗効果素子及びその製造方法が開 示されている。この磁気抵抗効果素子製造方法は、(A)真空容器の中で,反強磁性 層を基板の上面側に形成する工程と、(B)前記反強磁性層の形成の後、前記真空 容器に酸化性ガス (例示:酸素ガス)を導入する工程と、 (C)前記真空容器から前記 酸ィ匕性ガスを排気する工程と、(D)前記酸ィ匕性ガスの排気の後、前記反強磁性層の 上に、固定強磁性層を形成する工程と、(E)前記第 1強磁性層の上に、トンネルバリ ァ層を形成する工程と、(F)前記トンネルバリア層の上に、第 2強磁性層を形成する 工程とを含む。また、この磁気抵抗効果素子製造方法は、(G)反強磁性層を基板の 上面側に形成する工程と、(H)酸化性ガス (例示:酸素ガス)を含む雰囲気で、前記 反強磁性層の上に固定強磁性層を形成する工程と、(I)前記固定強磁性層の上に、 トンネルバリア層を形成する工程と、 ω前記トンネルバリア層の上に、自由強磁性層 を形成する工程とを含む。前記 (Η)工程の間の前記酸ィ匕性ガスの分圧は、形成され た前記第 1強磁性層が導電性を有するように定められて 、る。  [0013] In addition, Japanese Patent Application Laid-Open No. 2004-119903 discloses a magnetoresistive effect element and a method for manufacturing the same. This magnetoresistive element manufacturing method includes (A) a step of forming an antiferromagnetic layer on the upper surface side of a substrate in a vacuum container, and (B) after forming the antiferromagnetic layer, in the vacuum container. Introducing an oxidizing gas (e.g., oxygen gas), (C) exhausting the acidic gas from the vacuum vessel, and (D) exhausting the acidic gas, Forming a fixed ferromagnetic layer on the ferromagnetic layer; (E) forming a tunnel barrier layer on the first ferromagnetic layer; and (F) on the tunnel barrier layer. Forming a second ferromagnetic layer. Further, the magnetoresistive element manufacturing method includes (G) a step of forming an antiferromagnetic layer on the upper surface side of the substrate and (H) an antiferromagnetic layer in an atmosphere containing an oxidizing gas (eg, oxygen gas). Forming a fixed ferromagnetic layer on the layer; (I) forming a tunnel barrier layer on the fixed ferromagnetic layer; and ω forming a free ferromagnetic layer on the tunnel barrier layer. Including the step of. The partial pressure of the acidic gas during the step (ii) is determined so that the formed first ferromagnetic layer has conductivity.

[0014] また、特開 2000— 150984号公報に、オゾン酸化絶縁膜を使用した磁気トンネル 素子の技術が開示されている。このオゾン酸ィ匕絶縁膜を使用した磁気トンネル素子 は、保磁力が相互に異なる硬磁性膜及び軟磁性膜と、両者間に介在する絶縁膜とを 有する磁気トンネル素子にぉ ヽて、前記絶縁膜は酸素及びオゾンの混合気中で酸 化されたものである。  [0014] Further, Japanese Patent Application Laid-Open No. 2000-150984 discloses a technique of a magnetic tunnel element using an ozone oxidation insulating film. The magnetic tunnel element using the ozonate insulating film is a magnetic tunnel element having a hard magnetic film and a soft magnetic film having mutually different coercive forces, and an insulating film interposed between the two. The film is oxidized in a mixture of oxygen and ozone.

[0015] また、特開 2003— 258335号公報に、トンネル磁気抵抗効果素子の製造方法が 開示されている。これは、基板上に、第 1強磁性層、トンネル絶縁層、第 2強磁性層が この順に積層され、前記第 1強磁性層と第 2強磁性層の磁ィ匕方向の相対角度の違い によりトンネル磁気抵抗が異なるトンネル磁気抵抗効果素子の製造方法である。前記 トンネル絶縁層前駆体である導電層を形成する第 1工程と、前記導電層を酸素雰囲 気中で酸化させる第 2工程を含む。前記第 1工程において、前記導電層は 0. 4オン ダストローム Z秒以下の成膜速度で Al、 Mg、 Si、 Taの少なくとも 1種カゝら形成される 。前記第 1工程と前記第 2工程を複数回行うことによりトンネル絶縁層を形成しても良 い。前記第 2工程において真空中で酸ィ匕しても良ぐ酸化方法が自然酸化法、プラズ マ酸化法、ラジカル酸ィ匕法でも良い。 [0015] In addition, Japanese Unexamined Patent Application Publication No. 2003-258335 discloses a method for manufacturing a tunnel magnetoresistive effect element. This is because the first ferromagnetic layer, the tunnel insulating layer, and the second ferromagnetic layer are laminated in this order on the substrate, and the relative angle difference between the first ferromagnetic layer and the second ferromagnetic layer in the magnetic field direction is different. This is a method of manufacturing a tunnel magnetoresistive element having different tunnel magnetoresistance. A first step of forming a conductive layer as the tunnel insulating layer precursor; and a second step of oxidizing the conductive layer in an oxygen atmosphere. In the first step, the conductive layer is 0.4 on Dustrom At least one kind of Al, Mg, Si, Ta is formed at a deposition rate of Z seconds or less. The tunnel insulating layer may be formed by performing the first step and the second step a plurality of times. An oxidation method that can be oxidized in vacuum in the second step may be a natural oxidation method, a plasma oxidation method, or a radical oxidation method.

発明の開示  Disclosure of the invention

[0016] 従って、本発明の目的は、磁気トンネル接合におけるトンネルバリア層の品質を向 上することが可能な磁気抵抗効果素子及び磁気抵抗効果素子の製造方法、磁気ラ ンダムアクセスメモリを提供することにある。  Accordingly, an object of the present invention is to provide a magnetoresistive element capable of improving the quality of a tunnel barrier layer in a magnetic tunnel junction, a method for manufacturing the magnetoresistive element, and a magnetic random access memory. It is in.

[0017] また、本発明の他の目的は、磁気トンネル接合におけるネールカップリング磁界を ゼロにすることが可能な磁気抵抗効果素子及び磁気抵抗効果素子の製造方法、磁 気ランダムアクセスメモリを提供することにある。 [0017] Another object of the present invention is to provide a magnetoresistive effect element, a magnetoresistive effect element manufacturing method, and a magnetoresistive random access memory capable of making a nail coupling magnetic field in a magnetic tunnel junction zero. There is.

[0018] 本発明の更に他の目的は、磁気トンネル接合の特性を向上することが可能な磁気 抵抗効果素子及び磁気抵抗効果素子の製造方法、磁気ランダムアクセスメモリを提 供することにある。 Still another object of the present invention is to provide a magnetoresistive effect element capable of improving the characteristics of the magnetic tunnel junction, a method for manufacturing the magnetoresistive effect element, and a magnetic random access memory.

[0019] 本発明の別の目的は、製造歩留まりを改善することが可能な磁気抵抗効果素子及 び磁気抵抗効果素子の製造方法、磁気ランダムアクセスメモリを提供することにある  Another object of the present invention is to provide a magnetoresistive effect element capable of improving the manufacturing yield, a magnetoresistive effect element manufacturing method, and a magnetic random access memory.

[0020] 本発明の観点では、磁気抵抗効果素子の製造方法は、反強磁性層を基板の上面 側に形成することと、基板の上面側の反強磁性層の上に第 1固定強磁性層を形成す ることと、第 1固定強磁性層を 5 X 10_7Pa以上 1 X 10_4Pa以下の圧力で酸素原子を 含む気体に暴露を行うことと、第 1固定強磁性層の上に第 2固定強磁性層を形成す ることと、第 2固定強磁性層の上にトンネルバリア層を形成することと、トンネルバリア 層の上に自由強磁性層を形成することとにより達成される。ただし、酸素原子を含む 気体は、 5 X 10_7Pa以上 1 X 10_4Pa以下の圧力(又は分圧)の酸素ガスに例示さ れる。上記の磁気抵抗効果素子の製造方法において、第 2固定強磁性層の膜厚は 、 0より大きく lnm以下であるように形成される。 In the aspect of the present invention, the method of manufacturing a magnetoresistive element includes forming an antiferromagnetic layer on the upper surface side of the substrate, and forming a first fixed ferromagnetic layer on the antiferromagnetic layer on the upper surface side of the substrate. Forming a layer, exposing the first pinned ferromagnetic layer to a gas containing oxygen atoms at a pressure of 5 X 10 _7 Pa or more and 1 X 10 _4 Pa or less, and Forming a second pinned ferromagnetic layer on the first layer, forming a tunnel barrier layer on the second pinned ferromagnetic layer, and forming a free ferromagnetic layer on the tunnel barrier layer. The However, the gas containing oxygen atoms is exemplified by oxygen gas having a pressure (or partial pressure) of 5 × 10 _7 Pa or more and 1 × 10 _4 Pa or less. In the above magnetoresistive element manufacturing method, the second pinned ferromagnetic layer is formed so that the film thickness is greater than 0 and less than or equal to 1 nm.

[0021] また、本発明の他の観点では、磁気抵抗効果素子の製造方法は、反強磁性層を 基板の上面側に形成することと、反強磁性層の上に第 1固定強磁性層を形成するこ とと、第 1固定強磁性層を 5 X 10_7Pa以上 1 X 10_4Pa未満の圧力で酸素原子を含 む気体に暴露を行うことと、第 1固定強磁性層の上にトンネルバリア層を形成すること と、トンネルバリア層の上に自由強磁性層を形成することとにより達成される。ただし、 酸素原子を含む気体は、 5 X 10_7Pa以上 1 X 10_4Pa未満の圧力(又は分圧)の酸 素ガスに例示される。 [0021] In another aspect of the present invention, a method for manufacturing a magnetoresistive effect element includes: forming an antiferromagnetic layer on an upper surface side of a substrate; and a first fixed ferromagnetic layer on the antiferromagnetic layer. Forming And exposing the first pinned ferromagnetic layer to a gas containing oxygen atoms at a pressure of 5 X 10 _7 Pa or more and less than 1 X 10 _4 Pa, and a tunnel barrier layer on the first pinned ferromagnetic layer. And forming a free ferromagnetic layer on the tunnel barrier layer. However, a gas containing oxygen atoms is exemplified by an oxygen gas having a pressure (or partial pressure) of 5 × 10 _7 Pa or more and less than 1 × 10 _4 Pa.

[0022] 上記の磁気抵抗効果素子の製造方法において、第 1固定強磁性層をその酸素原 子を含む気体に暴露を行う工程は、 1 X 10_6Pa以上 1 X 10_5Pa以下の圧力で酸素 原子を含む気体に暴露を行うことがより望ましい。また、その酸素原子を含む気体は 、酸素ガス、水、メタノール及びエタノールガスのうちの少なくとも一つを含む気体で あることが好ましい。第 1固定強磁性層力 CoFe、 NiFe、 CoFeB、 CoFeCrのうちの 一つを含む膜を備える。上記の磁気抵抗効果素子の製造方法において、トンネルバ リア層側の第 1固定強磁性層の表面粗さが、第 1固定強磁性層より下層の表面粗さよ り小さい。 [0022] In the method of manufacturing a magnetoresistive effect element, the step of exposing the first pinned ferromagnetic layer to a gas containing oxygen atoms is performed at a pressure of 1 X 10 _6 Pa or more and 1 X 10 _5 Pa or less. It is more desirable to expose to gases containing oxygen atoms. The gas containing oxygen atoms is preferably a gas containing at least one of oxygen gas, water, methanol, and ethanol gas. The first pinned ferromagnetic layer force includes a film containing one of CoFe, NiFe, CoFeB, and CoFeCr. In the method of manufacturing a magnetoresistive effect element described above, the surface roughness of the first pinned ferromagnetic layer on the tunnel barrier layer side is smaller than the surface roughness of the lower layer than the first pinned ferromagnetic layer.

[0023] また、本発明の他の観点では、磁気抵抗効果素子は、反強磁性層と、第 1固定強 磁性層と、第 2固定強磁性層と、トンネルバリア層と、自由強磁性層とを具備する。反 強磁性層は、基板の上面側に形成されている。前記第 1固定強磁性層は、反強磁性 層の上に形成されている。第 2固定強磁性層は、第 1固定強磁性層の上に形成され ている。トンネルバリア層は、第 2固定強磁性層の上に形成されている。自由強磁性 層は、トンネルバリア層の上に形成されている。第 1固定強磁性層の第 2固定強磁性 層側の表面の領域は、他の領域に比較して酸素濃度が高い。トンネルバリア層側の 第 1固定強磁性層の表面粗さが、第 1固定強磁性層より下層の表面粗さより小さい。 ここで、第 1固定強磁性層は、固定強磁性層 A、非磁性層及び固定強磁性層 Bとを 備え、非磁性層を介した反強磁性層カップリングにより固定強磁性層 Aと固定強磁性 層 B6の磁ィ匕の方向は反平行になっている。また、上記の磁気抵抗効果素子におい て、第 2固定強磁性層の膜厚は、 0より大きく lnm以下である。  In another aspect of the present invention, the magnetoresistive effect element includes an antiferromagnetic layer, a first pinned ferromagnetic layer, a second pinned ferromagnetic layer, a tunnel barrier layer, and a free ferromagnetic layer. It comprises. The antiferromagnetic layer is formed on the upper surface side of the substrate. The first pinned ferromagnetic layer is formed on the antiferromagnetic layer. The second pinned ferromagnetic layer is formed on the first pinned ferromagnetic layer. The tunnel barrier layer is formed on the second pinned ferromagnetic layer. The free ferromagnetic layer is formed on the tunnel barrier layer. The region of the surface of the first pinned ferromagnetic layer on the second pinned ferromagnetic layer side has a higher oxygen concentration than the other regions. The surface roughness of the first pinned ferromagnetic layer on the tunnel barrier layer side is smaller than the surface roughness of the layer below the first pinned ferromagnetic layer. Here, the first pinned ferromagnetic layer includes a pinned ferromagnetic layer A, a nonmagnetic layer, and a pinned ferromagnetic layer B, and is pinned with the pinned ferromagnetic layer A by antiferromagnetic layer coupling via the nonmagnetic layer. The direction of the magnetic field of the ferromagnetic layer B6 is antiparallel. In the above magnetoresistive element, the thickness of the second pinned ferromagnetic layer is greater than 0 and less than or equal to 1 nm.

[0024] また、本発明の他の観点では、磁気抵抗効果素子は、反強磁性層と、第 1固定強 磁性層と、トンネルバリア層と、自由強磁性層とを具備する。反強磁性層は、基板の 上面側に形成されている。第 1固定強磁性層は、反強磁性層の上に形成されている 。トンネルバリア層は、第 1固定強磁性層の上に形成されている。自由強磁性層は、ト ンネルバリア層の上に形成されている。トンネルバリア層側の第 1固定強磁性層の表 面粗さが、第 1固定強磁性層より下層の表面粗さより小さい。上記の磁気抵抗効果素 子において、第 1固定強磁性層力 CoFe、 NiFe、 CoFeB、 CoFeCrのうちの一つを 含む膜を備える。 In another aspect of the present invention, the magnetoresistive effect element includes an antiferromagnetic layer, a first pinned ferromagnetic layer, a tunnel barrier layer, and a free ferromagnetic layer. The antiferromagnetic layer is formed on the upper surface side of the substrate. The first pinned ferromagnetic layer is formed on the antiferromagnetic layer. . The tunnel barrier layer is formed on the first pinned ferromagnetic layer. The free ferromagnetic layer is formed on the tunnel barrier layer. The surface roughness of the first pinned ferromagnetic layer on the tunnel barrier layer side is smaller than the surface roughness of the layer below the first pinned ferromagnetic layer. The magnetoresistive element includes a film containing one of the first fixed ferromagnetic layer forces CoFe, NiFe, CoFeB, and CoFeCr.

[0025] また、本発明の他の観点では、磁気ランダムアクセスメモリは、複数のワード線と、 複数のビット線と、複数の磁気抵抗効果素子とを具備する。複数のワード線は、第 1 方向 (X方向)へ延伸している。複数のビット線は、第 1方向 (X方向)と実質的に垂直 な第 2方向 (Y方向)へ伸びている。複数の磁気抵抗効果素子は、複数のワード線と 複数のビット線との交点の各々に設けられ、上記各項のいずれか一項に記載されて いる。  In another aspect of the present invention, a magnetic random access memory includes a plurality of word lines, a plurality of bit lines, and a plurality of magnetoresistive elements. The plurality of word lines extend in the first direction (X direction). The plurality of bit lines extend in a second direction (Y direction) substantially perpendicular to the first direction (X direction). The plurality of magnetoresistive elements are provided at each of the intersections of the plurality of word lines and the plurality of bit lines, and are described in any one of the above items.

図面の簡単な説明  Brief Description of Drawings

[0026] [図 1]図 1は、本発明の磁気抵抗効果素子の第 1実施例の構成を示す断面図である  FIG. 1 is a cross-sectional view showing a configuration of a first embodiment of a magnetoresistive element of the present invention.

[図 2]図 2は、本発明の磁気抵抗効果素子の製造方法の第 1実施例を示す断面図で ある。 FIG. 2 is a cross-sectional view showing a first embodiment of a method for producing a magnetoresistive element of the present invention.

[図 3]図 3は、本発明の磁気抵抗効果素子の製造方法の第 1実施例を示す断面図で ある。  FIG. 3 is a cross-sectional view showing a first embodiment of a method for producing a magnetoresistive element of the present invention.

[図 4]図 4は、本発明の磁気抵抗効果素子の製造方法の第 1実施例を示す断面図で ある。  FIG. 4 is a cross-sectional view showing a first embodiment of a method for producing a magnetoresistive element of the present invention.

[図 5]図 5は、本発明の磁気抵抗効果素子の製造方法の第 1実施例を示す断面図で ある。  FIG. 5 is a cross-sectional view showing a first embodiment of a method for producing a magnetoresistive element of the present invention.

[図 6]図 6は、本発明の磁気抵抗効果素子の製造方法の第 1実施例を示す断面図で ある。  FIG. 6 is a cross-sectional view showing a first embodiment of a method for producing a magnetoresistive element of the present invention.

[図 7]図 7は、酸素ガス処理における処理条件とネールカップリング磁界との関係を示 すグラフである。  [FIG. 7] FIG. 7 is a graph showing the relationship between the processing conditions in the oxygen gas processing and the nail coupling magnetic field.

[図 8]図 8は、本発明の磁気抵抗効果素子の第 2実施例の構成を示す断面図である [図 9]図 9は、本発明の磁気抵抗効果素子の製造方法の第 2実施例を示す断面図で ある。 FIG. 8 is a cross-sectional view showing a configuration of a second embodiment of the magnetoresistance effect element of the present invention. FIG. 9 is a cross-sectional view showing a second embodiment of the method for producing a magnetoresistive element of the present invention.

[図 10]図 10は、本発明の磁気抵抗効果素子の製造方法の第 2実施例を示す断面図 である。  FIG. 10 is a cross-sectional view showing a second embodiment of the method for manufacturing a magnetoresistive element of the present invention.

[図 11]図 11は、本発明の磁気抵抗効果素子の製造方法の第 2実施例を示す断面図 である。  FIG. 11 is a cross-sectional view showing a second embodiment of the method for producing a magnetoresistive element of the present invention.

[図 12]図 12は、本発明の磁気抵抗効果素子の製造方法の第 2実施例を示す断面図 である。  FIG. 12 is a cross-sectional view showing a second embodiment of the method for producing a magnetoresistive element of the present invention.

[図 13]図 13は、本発明の磁気抵抗効果素子の製造方法の第 2実施例を示す断面図 である。  FIG. 13 is a cross-sectional view showing a second embodiment of the method for manufacturing a magnetoresistive element of the present invention.

[図 14]図 14は、本発明の磁気抵抗効果素子の製造方法の第 2実施例を示す断面図 である。  FIG. 14 is a cross-sectional view showing a second embodiment of the method for producing a magnetoresistive element of the present invention.

[図 15]図 15は、酸素ガス処理における処理条件とネールカップリング磁界との関係を 示すグラフである。  FIG. 15 is a graph showing the relationship between the processing conditions in the oxygen gas processing and the nail coupling magnetic field.

[図 16]図 16は、磁気抵抗効果素子の製造方法を用いて作製した磁気抵抗効果素子 の磁場 抵抗変化率を示すグラフである。  FIG. 16 is a graph showing the rate of change in magnetic field resistance of a magnetoresistive effect element manufactured by using the magnetoresistive effect element manufacturing method.

[図 17]図 17は、磁気抵抗効果素子の製造方法を用 ヽて作製した磁気抵抗効果素子 と従来方法で作製した磁気抵抗効果素子との MR比のバイアス電圧依存性を示すグ ラフである。  FIG. 17 is a graph showing the bias voltage dependence of the MR ratio between a magnetoresistive effect element manufactured using a magnetoresistive effect element manufacturing method and a magnetoresistive effect element manufactured using a conventional method. .

[図 18]図 18は、本発明の磁気抵抗効果素子を磁気ランダムアクセスメモリに適用し たメモリセルの構成を示す断面図である。  FIG. 18 is a cross-sectional view showing a configuration of a memory cell in which the magnetoresistive element of the present invention is applied to a magnetic random access memory.

[図 19]図 19は、メモリセルを用いた MRAMの構成を示すブロック図である。  FIG. 19 is a block diagram showing a configuration of an MRAM using memory cells.

発明を実施するための最良の形態  BEST MODE FOR CARRYING OUT THE INVENTION

[0027] 本願は、米国特許出願番号 10Z520, 652と 10Z702, 655に関連する。これら の出願の開示内容は、引用により本願に取り込まれる。 [0027] This application is related to US patent application numbers 10Z520, 652 and 10Z702,655. The disclosure content of these applications is incorporated herein by reference.

[0028] 以下、本発明の磁気抵抗効果素子及び磁気抵抗効果素子の製造方法、磁気ラン ダムアクセスメモリを、添付図面を参照して説明する。 Hereinafter, a magnetoresistive effect element, a magnetoresistive effect element manufacturing method, and a magnetic random access memory according to the present invention will be described with reference to the accompanying drawings.

[0029] [第 1実施例] 本発明の第 1実施例による磁気抵抗効果素子及び磁気抵抗効果素子の製造方法 を、添付図面を参照して説明する。 [0029] [First embodiment] A magnetoresistive effect element and a method of manufacturing the magnetoresistive effect element according to the first embodiment of the present invention will be described with reference to the accompanying drawings.

[0030] まず、本発明の第 1実施例による磁気抵抗効果素子の構成について説明する。こ こでは、磁気ランダムアクセスメモリ(MRAM)に適用した磁気抵抗効果素子につい て説明する。図 1は、本発明の磁気抵抗効果素子の第 1実施例の構成を示す断面図 である。磁気抵抗効果素子 30は、基板 20の上面側に設けられ、シード層 2、反強磁 性層 3、固定強磁性層 A4、非磁性膜 5、固定強磁性層層 B6、トンネルバリア層 7、自 由強磁性層 8、キャップ層 9とを具備する。基板 20側はシード層 2が下部電極 1に、反 対側はキャップ層 9が上部電極(図示されず)にそれぞれ接続されている。  First, the configuration of the magnetoresistance effect element according to the first example of the present invention will be described. Here, a magnetoresistive element applied to a magnetic random access memory (MRAM) will be described. FIG. 1 is a cross-sectional view showing the configuration of the first embodiment of the magnetoresistive element of the present invention. The magnetoresistive effect element 30 is provided on the upper surface side of the substrate 20, and includes a seed layer 2, an antiferromagnetic layer 3, a fixed ferromagnetic layer A4, a nonmagnetic film 5, a fixed ferromagnetic layer B6, a tunnel barrier layer 7, A free ferromagnetic layer 8 and a cap layer 9 are provided. The seed layer 2 is connected to the lower electrode 1 on the substrate 20 side, and the cap layer 9 is connected to the upper electrode (not shown) on the opposite side.

[0031] 基板 20は、半導体基板上に CMOSに例示される素子 (MRAM用)が形成された 基板である。下部電極 1は、基板 20の上面側に設けられている。下部電極 1としては 、例えば、 Ta、 TaN、 Rh、 Irのような導電性材料が用いられる。上部電極(図示され ず)も同様である。シード層 2は、下部電極 1の上に設けられている。シード層 2として は、例えば、 NiFe、 CoFe、 NiCr、 NiFeCrなどの材料が用いられる。反強磁性層 3 は、シード層 2の上に設けられている。反強磁性層 3としては、例えば、 IrMn、 FeMn 、 PtMn、 Ni02、 a—Fe203のような反強磁性体が用いられる。固定強磁性層 A4 は、反強磁性層 3の上に設けられている。固定強磁性層 A4としては、例えば、 CoFe 、 NiFe、 CoFeB、 CoFeCrのような強磁性体が用いられる。非磁性層 5は、固定強 磁性層 A4の上に設けられている。非磁性層 5としては、例えば、 Ru、 Cuのような非 磁性体が用いられる。固定強磁性層 B6は、非磁性層 5の上に設けられている。固定 強磁性層 B6としては、例えば、 CoFe, NiFe、 CoFeB、 CoFeCrのような強磁性体 が用いられる。トンネルバリア層 7を形成する前に、真空中に酸素原子を含む気体を 所定の圧力で導入して、その表面を暴露することにより、固定強磁性層 B6の表面に 酸素基が吸着する。酸素原子を含む気体としては、酸素ガス、メタノール、水、ェタノ ールなどが用いられる。  [0031] The substrate 20 is a substrate in which an element exemplified by CMOS (for MRAM) is formed on a semiconductor substrate. The lower electrode 1 is provided on the upper surface side of the substrate 20. As the lower electrode 1, for example, a conductive material such as Ta, TaN, Rh, Ir is used. The same applies to the upper electrode (not shown). The seed layer 2 is provided on the lower electrode 1. For the seed layer 2, for example, a material such as NiFe, CoFe, NiCr, or NiFeCr is used. The antiferromagnetic layer 3 is provided on the seed layer 2. As the antiferromagnetic layer 3, for example, an antiferromagnetic material such as IrMn, FeMn, PtMn, Ni02, or a-Fe203 is used. The fixed ferromagnetic layer A4 is provided on the antiferromagnetic layer 3. As the fixed ferromagnetic layer A4, for example, a ferromagnetic material such as CoFe, NiFe, CoFeB, or CoFeCr is used. The nonmagnetic layer 5 is provided on the pinned ferromagnetic layer A4. As the nonmagnetic layer 5, for example, a nonmagnetic material such as Ru or Cu is used. The fixed ferromagnetic layer B6 is provided on the nonmagnetic layer 5. As the fixed ferromagnetic layer B6, for example, a ferromagnetic material such as CoFe, NiFe, CoFeB, and CoFeCr is used. Before the tunnel barrier layer 7 is formed, an oxygen group is adsorbed on the surface of the fixed ferromagnetic layer B6 by introducing a gas containing oxygen atoms into a vacuum at a predetermined pressure and exposing the surface thereof. As the gas containing oxygen atoms, oxygen gas, methanol, water, ethanol and the like are used.

[0032] トンネルバリア層 7は、固定強磁性層 B6の上に設けられている。トンネルバリア層 7 は、例えば A1などを酸素ラジカル、酸素プラズマ、オゾンなどをもちいて酸ィ匕すること により形成される絶縁性の非磁性体である。自由強磁性層 8は、トンネルバリア層 7の 上に設けられている。自由強磁性層 8としては、例えば NiFe、 CoFeB、 CoFe、 CoF eCrのような強磁性体の単層膜あるいは積層膜が用いられる。キャップ層 9は、自由 強磁性層 8の上に設けられている。キャップ層 9としては、例えば Ta、 TaN、 Rh、 Irの ような導電性材料が用いられる。 [0032] The tunnel barrier layer 7 is provided on the fixed ferromagnetic layer B6. The tunnel barrier layer 7 is an insulating nonmagnetic material formed by, for example, oxidizing A1 using oxygen radicals, oxygen plasma, ozone, or the like. The free ferromagnetic layer 8 is composed of the tunnel barrier layer 7 It is provided above. As the free ferromagnetic layer 8, a single layer film or a laminated film of a ferromagnetic material such as NiFe, CoFeB, CoFe, and CoFeCr is used. The cap layer 9 is provided on the free ferromagnetic layer 8. For the cap layer 9, for example, a conductive material such as Ta, TaN, Rh, Ir is used.

[0033] 図 1において、各膜の凹凸は、意図的ではなく成膜時に自然にできる程度の一般 的な凹凸を示している。ただし、トンネルバリア層 7は、その自由強磁性層 8側の表面 の凹凸が減少し、平滑な層になっている。それに伴いその上の各層も平滑になって いる。 In FIG. 1, the unevenness of each film shows general unevenness that is not intentional and can be naturally formed during film formation. However, the tunnel barrier layer 7 is a smooth layer with reduced irregularities on the surface of the free ferromagnetic layer 8 side. Along with this, the layers above it have also become smooth.

[0034] 次に、本発明の第 1実施例による磁気抵抗効果素子の製造方法について説明する 。図 2〜図 6は、本発明の第 1実施例による磁気抵抗効果素子の製造方法を示す断 面図である。  Next, a method for manufacturing a magnetoresistive effect element according to the first embodiment of the present invention will be described. 2 to 6 are sectional views showing a method of manufacturing a magnetoresistive effect element according to the first embodiment of the present invention.

図 2を参照して、基板 1の上面側に下部電極 1、シード層 2、反強磁性層 3、固定強 磁性層 A4、非磁性層 5、及び、固定強磁性層 B6がこの順に成膜される。成膜は、ス ノッタ法、イオンビームスパッタ法などを用いて行われる。  Referring to FIG. 2, lower electrode 1, seed layer 2, antiferromagnetic layer 3, pinned ferromagnetic layer A4, nonmagnetic layer 5, and pinned ferromagnetic layer B6 are formed in this order on the upper surface of substrate 1. Is done. Film formation is performed using a notched method, an ion beam sputtering method, or the like.

[0035] 次に、図 3を参照して、真空中に酸素ガス (又は同じ分圧で酸素ガスを含むガス)を 導入することにより、固定強磁性層 B6の表面を酸素ガスに暴露して、その表面に酸 素を吸着させる。このとき、図 7を参照して後述するように、酸素ガスの圧力(分圧)を 非常に小さくする。それにより、固定強磁性層 B6の表面は、酸素が吸着しているだけ 、又は、酸素を多く含む極めて薄い層があるだけで、固定強磁性層 B6の酸ィ匕層は無 い。酸素ガスでなぐメタノール、水、エタノールのような OH基を含む物質や、酸素 ガス、メタノール、水、エタノールのうちの二つ以上を組み合わせた気体でも良い。上 記の方法により、トンネルバリア層用の膜 7aの成膜の際、トンネルバリア層用膜 7aの 固定強磁性層 B6に対する濡れ性が向上し、薄くても連続した、ピンホールの無い膜 とすることが可能となる。  Next, referring to FIG. 3, by introducing oxygen gas (or a gas containing oxygen gas at the same partial pressure) into the vacuum, the surface of the fixed ferromagnetic layer B6 is exposed to oxygen gas. Adsorb oxygen on the surface. At this time, as will be described later with reference to FIG. 7, the pressure (partial pressure) of the oxygen gas is made very small. Thereby, the surface of the pinned ferromagnetic layer B6 has only oxygen adsorbed or has an extremely thin layer containing a large amount of oxygen, and there is no oxide layer of the pinned ferromagnetic layer B6. It may be a substance containing an OH group such as methanol, water, and ethanol, or a gas combining two or more of oxygen gas, methanol, water, and ethanol. By the above method, when the film 7a for the tunnel barrier layer is formed, the wettability of the tunnel barrier layer film 7a to the fixed ferromagnetic layer B6 is improved. It becomes possible to do.

[0036] 図 4を参照して、表面処理後の固定強磁性層 B6の上にトンネルバリア用膜 7aを成 膜する。成膜は、スパッタ法、イオンビームスパッタ法などを用いて行われる。上述の ように、トンネルバリア用膜 7aは、薄くても連続した、ピンホールの無い膜となる。この とき、膜の表面粗さ(平均表面粗さ Ra、最大の表面粗さ Rmax)が減少し、凹凸の少 ない膜となる。それと共に、表面粗さの周期が、固定強磁性層 B6などの下層の表面 のうねりに従わず、うねり周期が短くなる。 Referring to FIG. 4, tunnel barrier film 7a is formed on fixed ferromagnetic layer B6 after the surface treatment. Film formation is performed using a sputtering method, an ion beam sputtering method, or the like. As described above, the tunnel barrier film 7a is a continuous film without pinholes even if it is thin. At this time, the surface roughness of the film (average surface roughness Ra, maximum surface roughness Rmax) decreases, and the unevenness is reduced. There will be no film. At the same time, the period of the surface roughness does not follow the undulation of the surface of the lower layer such as the fixed ferromagnetic layer B6, and the undulation period becomes shorter.

[0037] 図 5を参照して、酸素プラズマを用いてトンネルバリア層用膜 7aが酸ィ匕される。酸素 プラズマの代わりに酸素ラジカル、オゾンなどを用いて酸ィ匕しても良い。それにより、ト ンネルバリア層用膜 7aは、酸ィ匕されて絶縁性のトンネルバリア層 7となる。トンネルバ リア層 7は、薄くても連続した、ピンホールの無い層となる。  Referring to FIG. 5, tunnel barrier layer film 7a is oxidized using oxygen plasma. Instead of oxygen plasma, oxygen radicals or ozone may be used for oxidation. As a result, the tunnel barrier layer film 7 a is oxidized and becomes an insulating tunnel barrier layer 7. The tunnel barrier layer 7 is a thin, continuous layer without pinholes.

[0038] 図 6を参照して、トンネルバリア層 7の上に自由強磁性層 8及びキャップ層 9がこの 順で成膜される。その後、図示しない上部電極が形成される。  Referring to FIG. 6, a free ferromagnetic layer 8 and a cap layer 9 are formed in this order on the tunnel barrier layer 7. Thereafter, an upper electrode (not shown) is formed.

[0039] 以上のように磁気抵抗効果素子の製造方法が実施される。なお、図 2、図 4〜図 6 の工程は、当業者にとって周知な他の方法を用いることも可能である。  As described above, the manufacturing method of the magnetoresistive effect element is performed. In addition, the method of FIG. 2, FIG. 4-6 can also use the other method well-known to those skilled in the art.

[0040] 図 7は、図 3の酸素ガス処理における処理条件とネールカップリング磁界との関係を 示すグラフである。縦軸はネールカップリング磁界の大きさ(Oe)、横軸は酸素暴露 時間 (秒)である。グラフ中の各曲線は、それぞれ異なる酸素ガス圧力(酸素ガス分圧 )の場合を示す。酸素ガス圧は、菱形が l X 10_7Pa、四角が l X 10_6Pa、三角が 1 X 10_5Pa、バッが 1 X 10_4Paである。図 7に示されるように、酸素ガス圧力が 1 X 10 _7Pa以上、 1 X 10_4Pa未満の間の非常に低い圧力範囲にあるとき、ネールカツプリ ング磁界が 0になる条件があることが分かる。すなわち、酸素ガス圧力は 1 X 10"7Pa 以上、 1 X 10_4Pa未満が好ましい。ただし、酸素ガス圧力の調整のしゃすさという面 から、 l X 10_6Pa以上、 l X 10_5Pa以下のガス圧が製造上より好ましい。 FIG. 7 is a graph showing the relationship between the processing conditions in the oxygen gas processing of FIG. 3 and the nail coupling magnetic field. The vertical axis is the magnitude of the nail coupling magnetic field (Oe), and the horizontal axis is the oxygen exposure time (seconds). Each curve in the graph shows a case of different oxygen gas pressure (oxygen gas partial pressure). Oxygen gas pressure, diamonds l X 10 _7 Pa, square l X 10 _6 Pa, triangle 1 X 10 _5 Pa, back is 1 X 10 _4 Pa. As shown in Fig. 7, when the oxygen gas pressure is in a very low pressure range between 1 X 10 _ 7 Pa and less than 1 X 10 _4 Pa, there may be a condition that the Neel coupling magnetic field becomes 0. I understand. That is, the oxygen gas pressure is preferably 1 X 10 " 7 Pa or more and less than 1 X 10 _4 Pa. However, from the aspect of adjusting the oxygen gas pressure, l X 10 _6 Pa or more and l X 10 _5 Pa or less The gas pressure is more preferable in production.

[0041] 図 3における酸素ガスの処理において、暴露する酸素雰囲気の酸素ガスの圧力を 変えることで、固定強磁性層 B6の表面を、酸素が吸着した状態、又は、酸素を多く 含む極めて薄い層が形成された状態にすることができる。こうして固定強磁性層 B6 の表面の状態を変化させることにより、トンネルバリア層用膜 7aの固定強磁性層 B6 に対する濡れ性が向上し、薄くても連続した膜を形成することができる。すなわち、ト ンネルバリア層用膜 7aの成長の仕方を変えることができ、トンネルバリア層用膜 7aを 酸ィ匕することにより形成されるトンネルバリア層 7の上面の平坦性 (表面粗さ)を変える ことができる。それにより、ネールカップリング磁界の大きさを 0にすることができる。す なわち、酸素ガスの処理の条件を調整することによって、ネールカップリング磁界の 大きさを 0にすることができる。同様に、酸素ガス以外のメタノール、水、エタノールやIn the treatment of oxygen gas in FIG. 3, by changing the pressure of oxygen gas in the oxygen atmosphere to be exposed, the surface of the fixed ferromagnetic layer B6 is in a state where oxygen is adsorbed or an extremely thin layer containing a large amount of oxygen. Can be formed. By changing the surface state of the fixed ferromagnetic layer B6 in this way, the wettability of the tunnel barrier layer film 7a to the fixed ferromagnetic layer B6 is improved, and a continuous film can be formed even if it is thin. That is, the growth method of the tunnel barrier layer film 7a can be changed, and the flatness (surface roughness) of the tunnel barrier layer 7 formed by oxidizing the tunnel barrier layer film 7a can be changed. be able to. As a result, the magnitude of the nail coupling magnetic field can be reduced to zero. In other words, by adjusting the oxygen gas treatment conditions, The size can be set to zero. Similarly, methanol other than oxygen gas, water, ethanol and

、酸素ガス、メタノール、水、エタノールのうちの二つ以上を組み合わせた気体を用い た場合でも、処理の条件を調整することにより、ネールカップリング磁界の大きさを 0 にすることができる。この場合、気体の圧力は、例えば、その気体が含む酸素原子の 量力 1 X 10_7Pa以上 1 X 10_4Pa未満の圧力の酸素ガスが含む酸素原子の量と同 じになるように設定する。 Even when a gas that combines two or more of oxygen gas, methanol, water, and ethanol is used, the magnitude of the nail coupling magnetic field can be reduced to zero by adjusting the treatment conditions. In this case, the pressure of the gas is set to be the same as the amount of oxygen atoms contained in the oxygen gas having a pressure of 1 X 10 _7 Pa or more and less than 1 X 10 _4 Pa, for example. .

[0042] 本発明では、固定強磁性層 B6表面の酸素ガス処理により、トンネルバリア層 7の固 定強磁性層 B6側の表面及び自由強磁性層 8側の表面力 それぞれトンネルバリア 層 7にピンホールが発生しない程度の適正な表面粗さに調整されている。したがって 、本発明により、トンネルバリア層 7のピンホールの発生を抑えつつ、ネールカツプリ ング磁界の大きさを 0にすることが可能となる。  In the present invention, by the oxygen gas treatment of the surface of the pinned ferromagnetic layer B6, the surface force of the tunnel barrier layer 7 on the fixed ferromagnetic layer B6 side and the surface force on the free ferromagnetic layer 8 side are respectively pinned on the tunnel barrier layer 7. It is adjusted to an appropriate surface roughness that does not generate holes. Therefore, according to the present invention, the magnitude of the Neel coupling magnetic field can be reduced to 0 while suppressing the generation of pinholes in the tunnel barrier layer 7.

[0043] [第 2実施例]  [0043] [Second embodiment]

本発明の第 2実施例による磁気抵抗効果素子及び磁気抵抗効果素子の製造方法 を、添付図面を参照して説明する。  A magnetoresistive effect element and a magnetoresistive effect element manufacturing method according to a second embodiment of the present invention will be described with reference to the accompanying drawings.

[0044] まず、本発明の第 2実施例による磁気抵抗効果素子の構成について説明する。こ こでは、磁気ランダムアクセスメモリ(MRAM)に適用した磁気抵抗効果素子につい て説明する。図 8は、本発明の第 2実施例による磁気抵抗効果素子の構成を示す断 面図である。磁気抵抗効果素子 30aは、基板 20の上面側に設けられ、シード層 2、 反強磁性層 3、固定強磁性層 A4、非磁性膜 5、固定強磁性層層 B6、境界層 10、固 定強磁性層 Cl l、トンネルバリア層 7、自由強磁性層 8、キャップ層 9とを具備する。 基板 20側はシード層 2が下部電極 1に、反対側はキャップ層 9が上部電極(図示され ず)にそれぞれ接続されている。本実施例の磁気抵抗効果素子 30aは、固定強磁性 層層 B6とトンネルバリア層 7の間に、境界層 10及び固定強磁性層 CI 1を設けて 、る 点で第 1実施例と異なる。  First, the configuration of the magnetoresistive effect element according to the second example of the present invention will be described. Here, a magnetoresistive element applied to a magnetic random access memory (MRAM) will be described. FIG. 8 is a cross-sectional view showing the configuration of the magnetoresistive effect element according to the second exemplary embodiment of the present invention. The magnetoresistive effect element 30a is provided on the upper surface side of the substrate 20, and includes a seed layer 2, an antiferromagnetic layer 3, a fixed ferromagnetic layer A4, a nonmagnetic film 5, a fixed ferromagnetic layer B6, a boundary layer 10, and a fixed layer. A ferromagnetic layer Cl l, a tunnel barrier layer 7, a free ferromagnetic layer 8, and a cap layer 9. On the substrate 20 side, the seed layer 2 is connected to the lower electrode 1, and on the other side, the cap layer 9 is connected to the upper electrode (not shown). The magnetoresistive effect element 30a of this embodiment is different from that of the first embodiment in that a boundary layer 10 and a fixed ferromagnetic layer CI1 are provided between the fixed ferromagnetic layer B6 and the tunnel barrier layer 7.

[0045] 境界層 10は、固定強磁性層 C11を形成する前に、真空中に酸素原子を含む気体 を所定の圧力で導入して固定強磁性層 B6の表面を暴露することにより形成される。 このとき、図 15を参照して後述するように、酸素ガスの圧力(分圧)を非常に小さくす る。それにより、境界層 10は、固定強磁性層 B6表面の酸素吸着層、又は酸素を多く 含む極めて薄い(例示: 1〜2分子)層として形成され、固固定強磁性層 B6の酸ィ匕層 は存在しない。酸素原子を含む気体としては、酸素ガス、メタノール、水、エタノール などが用いられる。 [0045] Before forming the pinned ferromagnetic layer C11, the boundary layer 10 is formed by introducing a gas containing oxygen atoms into a vacuum at a predetermined pressure to expose the surface of the pinned ferromagnetic layer B6. . At this time, as will be described later with reference to FIG. 15, the pressure (partial pressure) of the oxygen gas is made very small. As a result, the boundary layer 10 has an oxygen adsorption layer on the surface of the pinned ferromagnetic layer B6, or a large amount of oxygen. It is formed as a very thin (including one to two molecules) layer, and there is no oxide layer of the fixed pinned ferromagnetic layer B6. As the gas containing oxygen atoms, oxygen gas, methanol, water, ethanol and the like are used.

[0046] 固定強磁性層 C11は、境界層 10の上に設けられている。固定強磁性層 C11として は、 CoFe、 NiFe、 CoFeB、 CoFeCrなどの強磁性体が用いられる。トンネルバリア 層 7を形成する前に、真空中に酸素原子を含む気体を所定の圧力で導入して固定 強磁性層 C11の表面を暴露することにより、表面に酸素基が吸着されても良い。酸 素原子を含む気体としては、酸素ガス、メタノール、水、エタノールなどが用いられる  The fixed ferromagnetic layer C11 is provided on the boundary layer 10. Ferromagnetic materials such as CoFe, NiFe, CoFeB, and CoFeCr are used for the fixed ferromagnetic layer C11. Before forming the tunnel barrier layer 7, an oxygen group may be adsorbed on the surface by introducing a gas containing oxygen atoms into a vacuum at a predetermined pressure to expose the surface of the fixed ferromagnetic layer C11. As gas containing oxygen atoms, oxygen gas, methanol, water, ethanol, etc. are used.

[0047] 他の層については、第 1実施例と同様であるのでその説明を省略する。 [0047] The other layers are the same as those in the first embodiment, and thus the description thereof is omitted.

[0048] 図 8において、各膜の凹凸は、意図的ではなく成膜時に自然にできる程度の一般 的な凹凸を示している。ただし、固定強磁性層 C11は、その自由強磁性層 8側の表 面の凹凸が減少し、平滑な層になっている。それに伴いその上の各層も平滑になつ ている。 [0048] In FIG. 8, the unevenness of each film indicates general unevenness that is not intentional and can be naturally formed during film formation. However, the pinned ferromagnetic layer C11 has a smooth surface with reduced surface irregularities on the free ferromagnetic layer 8 side. Along with this, the layers above it are also smooth.

[0049] 次に、本発明の第 2実施例による磁気抵抗効果素子の製造方法について説明する 。図 9〜図 14は、本発明の第 2実施例による磁気抵抗効果素子の製造方法を示す 断面図である。  Next, a method for manufacturing a magnetoresistive effect element according to the second embodiment of the present invention will be described. 9 to 14 are cross-sectional views showing a method of manufacturing a magnetoresistive effect element according to the second embodiment of the present invention.

図 9を参照して、基板 1の上面側に下部電極 1、シード層 2、反強磁性層 3、固定強 磁性層 A4、非磁性層 5、及び、固定強磁性層 B6がこの順に成膜される。成膜は、ス ノッタ法、イオンビームスパッタ法などを用いて行われる。  Referring to FIG. 9, lower electrode 1, seed layer 2, antiferromagnetic layer 3, pinned ferromagnetic layer A4, nonmagnetic layer 5, and pinned ferromagnetic layer B6 are formed in this order on the upper surface of substrate 1. Is done. Film formation is performed using a notched method, an ion beam sputtering method, or the like.

[0050] 図 10を参照して、真空中に酸素ガス (又は同じ分圧で酸素ガスを含むガス)を導入 することにより固定強磁性層 B6の表面が酸素ガスに暴露される。これにより、固定強 磁性層 B6の表面に境界層 10が形成される。境界層 10は、固定強磁性層 B6表面の 酸素吸着層、又は、酸素を多く含む極めて薄い層である。酸素ガスでなぐメタノール 、水、エタノールのような OH基を含む物質や、酸素ガス、メタノール、水、エタノー ルのうちの二つ以上を組み合わせた気体が使用されてもよい。この方法により、固定 強磁性層 C11の成膜の際、固定強磁性層 C11が境界層 10の表面力 結晶成長す ることになるので、固定強磁性層 C11の境界層 10 (固定強磁性層 B6)に対する濡れ 性が向上する。また、その結晶状態は、固定強磁性層 B6のうえに直接形成される場 合とは異なる。 Referring to FIG. 10, the surface of fixed ferromagnetic layer B6 is exposed to oxygen gas by introducing oxygen gas (or a gas containing oxygen gas at the same partial pressure) into a vacuum. As a result, the boundary layer 10 is formed on the surface of the pinned ferromagnetic layer B6. The boundary layer 10 is an oxygen adsorption layer on the surface of the fixed ferromagnetic layer B6 or an extremely thin layer containing a large amount of oxygen. A substance containing an OH group such as methanol, water, ethanol, or a gas combining two or more of oxygen gas, methanol, water, and ethanol may be used. By this method, when the pinned ferromagnetic layer C11 is formed, the pinned ferromagnetic layer C11 grows by surface force of the boundary layer 10, so that the boundary layer 10 of the pinned ferromagnetic layer C11 (pinned ferromagnetic layer) B6) Improves. Also, the crystalline state is different from that formed directly on the pinned ferromagnetic layer B6.

[0051] 図 11を参照して、境界層 10の上に固定強磁性層 C11が成膜される。成膜は、スパ ッタ法、イオンビームスパッタ法などを用いて行われる。上述のように、境界層 10の表 面状態は、通常の固定強磁性層 B6のそれとは異なるので、成膜された固定強磁性 層 C11の表面状態力 通常の固定強磁性層 B6の表面とは異なるものになる。このと き、膜の表面粗さ(平均表面粗さ Ra、最大の表面粗さ Rmax)が減少し、凹凸の少な い膜となる。それと共に、表面粗さの周期が下層(固定強磁性層 B6など)の表面のう ねりに従わず、うねり周期が短くなる。その結果、トンネルバリア層用膜 7aの成膜の際 、トンネルバリア層用膜 7aの固定強磁性層 C11に対する濡れ性が向上し、薄くても 連続した、ピンホールの無 、膜とすることが可能となる。  Referring to FIG. 11, the fixed ferromagnetic layer C11 is formed on the boundary layer 10. Film formation is performed using a sputtering method, an ion beam sputtering method, or the like. As described above, since the surface state of the boundary layer 10 is different from that of the normal pinned ferromagnetic layer B6, the surface state force of the formed pinned ferromagnetic layer C11 is different from that of the normal pinned ferromagnetic layer B6. Will be different. At this time, the surface roughness (average surface roughness Ra, maximum surface roughness Rmax) of the film decreases, and the film has less unevenness. At the same time, the period of the surface roughness does not follow the surface waviness of the lower layer (such as the fixed ferromagnetic layer B6), and the waviness period becomes shorter. As a result, when the tunnel barrier layer film 7a is formed, the wettability of the tunnel barrier layer film 7a with respect to the fixed ferromagnetic layer C11 is improved, and the film can be made continuous even without being thin and without pinholes. It becomes possible.

[0052] 図 12を参照して、固定強磁性層 C11の上にトンネルバリア層用膜 7aが成膜される 。成膜は、スパッタ法、イオンビームスパッタ法などを用いて行われる。上述のように、 トンネルバリア層用膜 7aは、薄くても連続した、ピンホールの無い膜となる。図 13を参 照して、酸素プラズマを用いてトンネルバリア用膜 7aは酸ィ匕される。酸素プラズマの 代わりに酸素ラジカル、オゾンなどを用いて酸ィ匕されても良い。それ〖こより、トンネル ノリア用膜 7aは、酸化され、絶縁性のトンネルバリア層 7となる。トンネルバリア層 7は 、薄くても連続したピンホールの無い層となる。  Referring to FIG. 12, tunnel barrier layer film 7a is formed on fixed ferromagnetic layer C11. Film formation is performed using a sputtering method, an ion beam sputtering method, or the like. As described above, the tunnel barrier layer film 7a is a continuous film that does not have pinholes even if it is thin. Referring to FIG. 13, tunnel barrier film 7a is oxidized using oxygen plasma. Instead of oxygen plasma, oxygen radicals or ozone may be used for oxidation. Accordingly, the tunnel noria film 7a is oxidized to become an insulating tunnel barrier layer 7. The tunnel barrier layer 7 is a thin layer without a continuous pinhole.

[0053] 図 14を参照して、トンネルバリア層 7の上に自由強磁性層 8及びキャップ層 9がこの 順で成膜される。その後、図示しない上部電極を形成する。  Referring to FIG. 14, a free ferromagnetic layer 8 and a cap layer 9 are formed in this order on the tunnel barrier layer 7. Thereafter, an upper electrode (not shown) is formed.

[0054] 以上のように磁気抵抗効果素子の製造方法が実施される。なお、図 9、図 12〜図 1 4の工程は、当業者にとって周知な他の方法を用いることも可能である。この製法に おいて、図 11における残りの固定強磁性層 C11を成膜する際に、酸素原子を含む ガス雰囲気中で成膜を行うことによつても、同じ効果を得ることができる。  As described above, the method for manufacturing a magnetoresistive element is performed. In addition, the method of FIG. 9, FIG. 12-FIG. 14 can also use the other method well-known to those skilled in the art. In this manufacturing method, the same effect can be obtained by forming the remaining pinned ferromagnetic layer C11 in FIG. 11 in a gas atmosphere containing oxygen atoms.

[0055] 図 15は、図 10の酸素ガス処理における処理条件とネールカップリング磁界との関 係を示すグラフである。縦軸はネールカップリング磁界の大きさ(Oe)、横軸は固定強 磁性層 C11の膜厚 (nm)である。グラフ中の各曲線は、それぞれ異なる酸素ガス圧 力(酸素ガス分圧)の場合を示す。酸素ガス圧は、菱形が l X 10_7Pa、四角が 1 X 1 0_bPa、三角が 1 X 10_4Pa、バッが 1 X 10_dPaである。酸素暴露時間は、 240秒で ある。 FIG. 15 is a graph showing the relationship between processing conditions and the nail coupling magnetic field in the oxygen gas processing of FIG. The vertical axis is the magnitude of the nail coupling magnetic field (Oe), and the horizontal axis is the film thickness (nm) of the fixed ferromagnetic layer C11. Each curve in the graph shows the case of different oxygen gas pressure (oxygen gas partial pressure). Oxygen gas pressure is l X 10 _7 Pa for diamond and 1 X 1 for square 0 _b Pa, the triangle is 1 X 10 _4 Pa, and the back is 1 X 10 _d Pa. The oxygen exposure time is 240 seconds.

[0056] 図 15に示されるように、固定層強磁性層 C11の膜厚が 0より大きく lnm以下の範囲 において、酸素ガス圧力が 1 X 10_7Pa以上、 1 X 10_3Pa未満の間の非常に低い圧 力範囲にあるとき、ネールカップリング磁界が 0になる条件があることが分かる。すな わち、酸素ガス圧力は 1 X 10_7Pa以上、 1 X 10_4Pa以下が好ましい。ただし、酸素 ガス圧力の調整のしゃすさという面から、 l X 10_6Pa以上、 1 X 10_5Pa以下のガス 圧が製造上より好ましい。固定層強磁性層 C11の膜厚が lnmより大きい場合、ネー ルカップリング磁界が 0になる点はな 、。 [0056] As shown in FIG. 15, when the film thickness of the fixed layer ferromagnetic layer C11 is greater than 0 and less than or equal to 1 nm , the oxygen gas pressure is between 1 X 10 _7 Pa and less than 1 X 10 _3 Pa. It can be seen that there is a condition where the nail coupling magnetic field is zero when in the very low pressure range. That is, the oxygen gas pressure is preferably 1 × 10 _7 Pa or more and 1 × 10 _4 Pa or less. However, a gas pressure of 1 × 10_6 Pa or more and 1 × 10_5 Pa or less is preferable from the viewpoint of adjustment of oxygen gas pressure. When the film thickness of the fixed layer ferromagnetic layer C11 is greater than lnm, the nail coupling magnetic field is zero.

[0057] 図 10における酸素ガスの処理において、暴露する酸素雰囲気の酸素ガスの圧力 を変えることで、固定強磁性層 B6表面の酸素吸着層、または、極めて薄い固定強磁 性層 B6の酸ィ匕層である境界層 10を形成することができる。また、固定強磁性層 B6 の表面の状態を境界層 10で変化させることにより、固定強磁性層 C11の結晶状態を 変化させることができる。固定強磁性層 C11の表面状態が変化するので、トンネルバ リア層用膜 7aの成膜の際、トンネルバリア層用膜 7aが固定強磁性層 C11の表面力 結晶成長しやすくなり、薄くても連続した膜を形成することができる。すなわち、トンネ ルバリア層用膜 7aの成長の仕方を変化させることができ、トンネルバリア層用膜 7aを 酸ィ匕することにより形成されるトンネルバリア層 7の上面の平坦性を変化させることが できる。それにより、ネールカップリング磁界の大きさを 0にすることができる。すなわ ち、酸素ガスの処理の条件を調整することによって、ネールカップリング磁界の大きさ を 0にすることができる。同様に、酸素ガス以外のメタノール、水、エタノールや、酸素 ガス、メタノール、水、エタノールのうちの二つ以上を組み合わせたものを用いた場合 でも、処理の条件を調整することにより、ネールカップリング磁界の大きさを 0にするこ とがでさる。  [0057] In the treatment of oxygen gas in FIG. 10, the oxygen adsorption layer on the surface of the fixed ferromagnetic layer B6 or the acid layer of the extremely thin fixed ferromagnetic layer B6 is changed by changing the pressure of the oxygen gas in the oxygen atmosphere to be exposed. It is possible to form the boundary layer 10 which is a soot layer. Further, by changing the surface state of the pinned ferromagnetic layer B6 at the boundary layer 10, the crystal state of the pinned ferromagnetic layer C11 can be changed. Since the surface state of the pinned ferromagnetic layer C11 changes, when the tunnel barrier layer film 7a is formed, the tunnel barrier layer film 7a has a surface force on the pinned ferromagnetic layer C11. Film can be formed. That is, the growth method of the tunnel barrier layer film 7a can be changed, and the flatness of the upper surface of the tunnel barrier layer 7 formed by oxidizing the tunnel barrier layer film 7a can be changed. . As a result, the magnitude of the nail coupling magnetic field can be reduced to zero. In other words, the magnitude of the nail coupling magnetic field can be reduced to zero by adjusting the conditions for treating oxygen gas. Similarly, even when using methanol, water, ethanol other than oxygen gas, or a combination of two or more of oxygen gas, methanol, water, and ethanol, nail coupling can be achieved by adjusting the processing conditions. It is possible to reduce the magnitude of the magnetic field to zero.

[0058] 本発明では、固定強磁性層 B6表面の酸素ガス処理により、トンネルバリア層 7の固 定強磁性層 B6側の表面及び自由強磁性層 8側の表面力 それぞれトンネルバリア 層 7にピンホールが発生しない程度の適正な表面粗さに調整されている。したがって 、本発明により、トンネルバリア層 7のピンホールの発生を抑えつつ、ネールカツプリ ング磁界の大きさを 0にすることが可能となる。このとき、固定強磁性層 B6の材料が 変わると酸素ガスの濡れ性等の変化により最適な酸素暴露条件が異なる。濡れ性の 良!ヽ材料であると酸素暴露時間は短くなり、濡れ性の悪 、材料だと酸素暴露時間は 長くなる。 In the present invention, by the oxygen gas treatment of the surface of the fixed ferromagnetic layer B 6, the surface force of the tunnel barrier layer 7 on the fixed ferromagnetic layer B 6 side and the surface force of the free ferromagnetic layer 8 side are respectively pinned on the tunnel barrier layer 7. It is adjusted to an appropriate surface roughness that does not generate holes. Therefore, according to the present invention, while preventing the generation of pinholes in the tunnel barrier layer 7, The magnitude of the magnetic field can be reduced to zero. At this time, if the material of the pinned ferromagnetic layer B6 is changed, the optimum oxygen exposure conditions differ depending on changes in the wettability of oxygen gas. Good wettability!ヽ Materials have a shorter oxygen exposure time and poor wettability, and materials have a longer oxygen exposure time.

[0059] 図 16は、上記製法 (第 1実施例又は第 2実施例)を用いて作製した磁気トンネル接 合の磁気抵抗効果素子の磁場 抵抗変化率を示すグラフである。縦軸は磁気抵抗 効果素子(MTJ膜)の磁気抵抗 (MR: Magnetic Resistance)変化率(%)、横軸 は磁気抵抗効果素子に印加する磁場の大きさ(Oe)である。トンネルバリア層 7が平 滑になった効果によりバイアス電圧 lOOmVにおいて約 40%の抵抗変化率が得られ た。  FIG. 16 is a graph showing the rate of change in magnetic field resistance of the magnetoresistive effect element in the magnetic tunnel junction manufactured by using the above manufacturing method (first example or second example). The vertical axis is the magnetoresistance (MR) change rate (%) of the magnetoresistive effect element (MTJ film), and the horizontal axis is the magnitude (Oe) of the magnetic field applied to the magnetoresistive effect element. Due to the effect of the smoothing of the tunnel barrier layer 7, a resistance change rate of about 40% was obtained at a bias voltage of lOOmV.

[0060] 図 17は、上記製法 (第 1実施例又は第 2実施例)を用いて作製した磁気抵抗効果 素子 (MTJ膜)(a)と従来方法で作製した磁気抵抗効果素子 (MTJ膜)(b)との MR 比 (抵抗変化率 (%) )のバイアス電圧依存性を示すグラフである。本発明を用いて作 製された磁気抵抗効果素子は、どのバイアス電圧にぉ ヽても従来の磁気抵抗効果 素子に比べて高い MR比が得られている。これは、トンネルバリア層 7 (アルミナ)の品 質が向上した結果である。すなわち、磁気抵抗効果素子の磁気トンネル接合におけ るトンネルバリア層の品質を向上し、ネールカップリング磁界をゼロにすることができ、 磁気抵抗効果素子の磁気トンネル接合の特性を向上することが可能となる。  FIG. 17 shows a magnetoresistive effect element (MTJ film) (a) manufactured using the above manufacturing method (first embodiment or second embodiment) (a) and a magnetoresistive effect element (MTJ film) manufactured by a conventional method. It is a graph which shows the bias voltage dependence of MR ratio (resistance change rate (%)) with (b). The magnetoresistive effect element manufactured using the present invention has a higher MR ratio than the conventional magnetoresistive effect element at any bias voltage. This is a result of the improved quality of the tunnel barrier layer 7 (alumina). In other words, the quality of the tunnel barrier layer in the magnetic tunnel junction of the magnetoresistive effect element can be improved, the nail coupling magnetic field can be made zero, and the characteristics of the magnetic tunnel junction of the magnetoresistive effect element can be improved. It becomes.

[0061] [第 3実施例]  [0061] [Third embodiment]

本発明の磁気抵抗効果素子及び磁気抵抗効果素子の製造方法を適用した磁気ラ ンダムアクセスメモリの実施例に関して、添付図面を参照して説明する。  Embodiments of a magnetic random access memory to which a magnetoresistive effect element and a method of manufacturing a magnetoresistive effect element according to the present invention are applied will be described with reference to the accompanying drawings.

[0062] まず、本発明の磁気抵抗効果素子を適用した磁気ランダムアクセスメモリの実施例 の構成について説明する。図 18は、本発明の磁気抵抗効果素子を磁気ランダムァク セスメモリに適用したメモリセルの構成を示す断面図である。メモリセル 42は、既述の 磁気抵抗効果素子 30 (又は 30a)、下部電極 1、上部電極 31、 MOSトランジスタ 46 、コンタクト配線 47、コンタクト配線 48を備える。メモリセル 42は、書き込みワード線 4 3、読み出しワード線 44、ビット線 45、 GND線 50に接続されている。  First, the configuration of an example of a magnetic random access memory to which the magnetoresistive effect element of the present invention is applied will be described. FIG. 18 is a cross-sectional view showing the configuration of a memory cell in which the magnetoresistive element of the present invention is applied to a magnetic random access memory. The memory cell 42 includes the magnetoresistive effect element 30 (or 30a), the lower electrode 1, the upper electrode 31, the MOS transistor 46, the contact wiring 47, and the contact wiring 48 described above. The memory cell 42 is connected to the write word line 43, the read word line 44, the bit line 45, and the GND line 50.

[0063] MOSトランジスタ 46は、半導体基板内に設けられた第 1拡散層 46aと、第 2拡散層 46cと、第 1拡散層 46aと第 2拡散層 46cとの間の半導体基板上に絶縁層を介して設 けられた第 1ゲート 46bとを含む。第 1拡散層 46aは、コンタクト配線 48を介して GND 線 50に接続されている。第 2拡散層 46cは、コンタクト配線 47を介して下部電極 1の 一端に接続されている。ゲート 46bは、読み出しワード線 44に接続されている。下部 電極 1は、他端において磁気抵抗効果素子 30 (、 30a)の一端側と接続されている。 磁気抵抗効果素子 30 (、 30a)は、第 1実施例又は第 2実施例で説明された磁気抵 抗効果素子 (磁気トンネル接合素子)である。磁気抵抗効果素子 30 (、 30a)は、他端 側において上部電極 31を介してビット線 45と接続されている。また、磁気抵抗効果 素子 30 (、 30a)に対して、ビット線 45と反対の側に下部電極 1及び層間絶縁層 49を 介して、ビット線 45と直交するように書き込みワード線 43が設けられている。 [0063] The MOS transistor 46 includes a first diffusion layer 46a and a second diffusion layer provided in the semiconductor substrate. 46c, and a first gate 46b provided on the semiconductor substrate between the first diffusion layer 46a and the second diffusion layer 46c via an insulating layer. The first diffusion layer 46 a is connected to the GND line 50 via the contact wiring 48. The second diffusion layer 46 c is connected to one end of the lower electrode 1 through the contact wiring 47. The gate 46b is connected to the read word line 44. The lower electrode 1 is connected to one end side of the magnetoresistive effect element 30 (30a) at the other end. The magnetoresistive effect element 30 (30a) is the magnetoresistive effect element (magnetic tunnel junction element) described in the first embodiment or the second embodiment. The magnetoresistive effect element 30 (30a) is connected to the bit line 45 via the upper electrode 31 on the other end side. A write word line 43 is provided on the opposite side to the bit line 45 with respect to the magnetoresistive effect element 30 (30a) via the lower electrode 1 and the interlayer insulating layer 49 so as to be orthogonal to the bit line 45. ing.

[0064] 磁気抵抗効果素子 30 (、 30a)における自由強磁性層 8の自発磁ィ匕は、メモリセル 4 2の上を通るビット線 45を流れる電流と、メモリセル 42の下を通る書き込みワード線 4 3に流れる電流とによって誘起される合成磁場によって、所望の向きに反転される。  [0064] In the magnetoresistive effect element 30 (30a), the spontaneous magnetization of the free ferromagnetic layer 8 includes the current flowing through the bit line 45 passing over the memory cell 42 and the write word passing under the memory cell 42. It is reversed in the desired orientation by the resultant magnetic field induced by the current flowing in line 43.

[0065] 図 19は、メモリセル 42を用いた MRAM60の構成を示すブロック図である。この M RAM60は、複数のメモリセル 42、複数の参照用メモリセル 42r、複数の書き込みヮ ード線 43、複数の読み出しワード線 44、複数のビット線 45、 Xセレクタ 58、 X側電流 源回路 59、 X側電流終端回路 56、 Yセレクタ 51、 Y側電流源回路 52、読み出し電 流負荷回路 53、 Y側電流終端回路 54及びセンスアンプ 55を具備する。  FIG. 19 is a block diagram showing a configuration of the MRAM 60 using the memory cell 42. The MRAM 60 includes a plurality of memory cells 42, a plurality of reference memory cells 42r, a plurality of write word lines 43, a plurality of read word lines 44, a plurality of bit lines 45, an X selector 58, and an X-side current source circuit. 59, an X side current termination circuit 56, a Y selector 51, a Y side current source circuit 52, a read current load circuit 53, a Y side current termination circuit 54, and a sense amplifier 55.

[0066] メモリセル 42は、複数の書き込みワード線 43 (複数の読み出しワード線 44)と複数 のビット線 45との交点の各々に対応して設けられ、行列に配列されている。 Xセレクタ 58は、 X軸方向(ワード線方向)に延設されている複数の読み出しワード線 44及び複 数の書き込みワード線 43から、読み出し動作時には所望の選択読み出しワード線 4 4sを、書き込み動作時には所望の選択書き込みワード線 43sを選択する。 X側電流 源回路 59は、メモリセル 42へのデータ書き込み動作時に、定電流を供給する定電 流源である。 X側電流終端回路 56は、複数の書き込みワード線 43を終端する。 Yセ レクタ 51は、 Y軸方向(ビット線方向)に延設されている複数のビット線 45から、所望 の選択ビット線 45sを選択する。 Y側電流源回路 52は、メモリセル 42へのデータ書き 込み動作時に、定電流を供給する定電流源である。読み出し電流負荷回路 53は、メ モリセル 42からのデータ読み出し動作時に、選択されたメモリセル 42 (以下、選択セ ル 42s)と、リファレンス用のメモリセル 42rに所定の電流を供給する定電流源である。 Y側電流終端回路 54は、複数のビット線 45を終端する。センスアンプ 55は、リファレ ンス用のメモリセル 42rにつながるリファレンス用のビット線 45rの電圧と、選択セル 4 2sにつながるビット線 45の電圧との差に基づいて、選択セル 42sのデータを出力す る。 [0066] The memory cells 42 are provided corresponding to the intersections of the plurality of write word lines 43 (the plurality of read word lines 44) and the plurality of bit lines 45, and are arranged in a matrix. The X selector 58 writes a desired selected read word line 44 s during a read operation from a plurality of read word lines 44 and a plurality of write word lines 43 extending in the X-axis direction (word line direction). Sometimes the desired selective write word line 43s is selected. The X-side current source circuit 59 is a constant current source that supplies a constant current during a data write operation to the memory cell 42. The X-side current termination circuit 56 terminates the plurality of write word lines 43. The Y selector 51 selects a desired selected bit line 45s from the plurality of bit lines 45 extending in the Y-axis direction (bit line direction). The Y-side current source circuit 52 is a constant current source that supplies a constant current during a data write operation to the memory cell 42. Read current load circuit 53 This is a constant current source that supplies a predetermined current to the selected memory cell 42 (hereinafter, selected cell 42 s) and the reference memory cell 42 r during the data read operation from the memory cell 42. The Y side current termination circuit 54 terminates the plurality of bit lines 45. The sense amplifier 55 outputs the data of the selected cell 42s based on the difference between the voltage of the reference bit line 45r connected to the memory cell 42r for reference and the voltage of the bit line 45 connected to the selected cell 42s. The

[0067] メモリセル 42からのデータの読み出しは、以下のようにして行う。すなわち、 Xセレク タ 58で選択された選択読み出しワード線 44sと、 Yセレクタ 51で選択された選択ビッ ト線 45sとの交点に対応する選択セル 42sの磁気抵抗効果素子 30 (、 30a)に対して 、読み出し電流負荷回路 53により定電流が供給される。それにより、選択ビット線 45 sが、磁気抵抗効果素子 30 (、 30a)の自由強磁性層 8の状態 (磁気抵抗効果素子 3 0 (、 30a)の抵抗値)に対応した大きさを有する電圧となる。一方、ビット線 45rと選択 読み出しワード線 44sとで選択されるリファレンス用のメモリセル 42rに対しても、同様 に定電流が供給され、ビット線 45r力 所定のリファレンス電圧となる。そして、センス アンプ 55は、両電圧の大きさを比較し、例えば、選択ビット線 45sの電圧がリファレン ス電圧より大きければ選択セル 42sのデータは「1」、小さければ「0」と判定する。  [0067] Reading data from the memory cell 42 is performed as follows. That is, for the magnetoresistive effect element 30 (30a) of the selected cell 42s corresponding to the intersection of the selected read word line 44s selected by the X selector 58 and the selected bit line 45s selected by the Y selector 51 Thus, a constant current is supplied by the read current load circuit 53. As a result, the selected bit line 45 s has a voltage corresponding to the state of the free ferromagnetic layer 8 of the magnetoresistive element 30 (30a) (the resistance value of the magnetoresistive element 30 (30a)). It becomes. On the other hand, a constant current is similarly supplied to the reference memory cell 42r selected by the bit line 45r and the selected read word line 44s, and the bit line 45r has a predetermined reference voltage. Then, the sense amplifier 55 compares the magnitudes of the two voltages. For example, if the voltage of the selected bit line 45s is greater than the reference voltage, the data of the selected cell 42s is determined to be “1”, and if it is smaller, “0”.

[0068] メモリセル 42へのデータの書き込みは、以下のようにして行う。すなわち、 Xセレクタ 58で選択された選択書き込みワード線 43sと、 Yセレクタ 51で選択された選択ビット 線 45sとの交点に対応する選択セル 42sの磁気抵抗効果素子 30 (、 30a)に対して、 Y方向の磁界 Hと X方向の磁界 Hとが発生される。これにより、合成磁界 Hが生成さ  [0068] Data is written to the memory cell 42 as follows. That is, for the magnetoresistive effect element 30 (30a) of the selected cell 42s corresponding to the intersection of the selected write word line 43s selected by the X selector 58 and the selected bit line 45s selected by the Y selector 51, A magnetic field H in the Y direction and a magnetic field H in the X direction are generated. As a result, a composite magnetic field H is generated.

Y X  Y X

れる。ただし、磁界 Hは、選択書き込みワード線 43sに、 X側電流源回路 59により電  It is. However, the magnetic field H is applied to the selective write word line 43s by the X-side current source circuit 59.

Y  Y

流が流されることにより発生する。また、磁界 Hは、選択ビット線 45sに、 Y側電流源  It is generated by flowing a flow. The magnetic field H is applied to the Y-side current source on the selected bit line 45s.

X  X

回路 52により書き込むデータに対応した向きを有する電流が流されることにより発生 する。磁気抵抗効果素子 30 (、 30a)は、合成磁界 Hを受け、書き込むデータに対応 するように自発磁化の方向を反転する。  It is generated when a current having a direction corresponding to the data written by the circuit 52 flows. The magnetoresistive effect element 30 (30a) receives the combined magnetic field H and reverses the direction of spontaneous magnetization so as to correspond to the data to be written.

[0069] 第 1実施例及び第 2実施例の磁気抵抗効果素子を用いることで、磁気抵抗効果素 子の磁気トンネル接合におけるトンネルバリア層の品質を向上し、ネールカップリング 磁界をゼロにすることができ、磁気抵抗効果素子の磁気トンネル接合の特性を向上 することが可能となる。そして、この磁気抵抗効果素子を磁気ランダムアクセスメモリ に用いることで、磁気ランダムアクセスメモリの製造歩留まりを改善することが可能とな る。 [0069] By using the magnetoresistive effect element of the first and second embodiments, the quality of the tunnel barrier layer in the magnetic tunnel junction of the magnetoresistive effect element is improved, and the nail coupling magnetic field is made zero. Can improve the characteristics of the magnetic tunnel junction of the magnetoresistive effect element It becomes possible to do. By using this magnetoresistive element for a magnetic random access memory, it becomes possible to improve the manufacturing yield of the magnetic random access memory.

[0070] 本発明により、トンネルバリア層の上下の面を平滑とすることができ、トンネルバリア 層の品質を向上し、高 MRな MRAMを製造することができる。そして、ネールカップ リング磁界を 0とすることでオフセット磁界を 0に容易に調整することができる。その結 果、メモリセル 42間のディスターブに強ぐ書込み電流を低く抑えた MRAMを製造 することが可能となる。  [0070] According to the present invention, the upper and lower surfaces of the tunnel barrier layer can be made smooth, the quality of the tunnel barrier layer can be improved, and a high MR MRAM can be manufactured. The offset magnetic field can be easily adjusted to zero by setting the nail coupling magnetic field to zero. As a result, it is possible to manufacture an MRAM in which the write current that is strong against the disturbance between the memory cells 42 is kept low.

[0071] また、本発明の磁気抵抗効果素子は、 MRAMのほかに、磁気ディスク装置の磁気 ヘッドなどいおいて起用することも可能である。本発明により、磁気トンネル接合にお けるネールカップリング磁界をゼロにし、トンネルバリア層の品質を向上させることが できる。  In addition to the MRAM, the magnetoresistance effect element of the present invention can also be used in a magnetic head of a magnetic disk device. According to the present invention, the nail coupling magnetic field in the magnetic tunnel junction can be made zero, and the quality of the tunnel barrier layer can be improved.

Claims

請求の範囲 The scope of the claims [1] 基板の上面側に反強磁性層を形成する工程と、  [1] forming an antiferromagnetic layer on the upper surface side of the substrate; 前記反強磁性層の上に第 1固定強磁性層を形成する工程と、  Forming a first pinned ferromagnetic layer on the antiferromagnetic layer; 前記第 1固定強磁性層を 5 X 10_7Pa以上 1 X 10_4Pa以下の圧力で酸素原子を含 む気体に暴露を行う工程と、 Exposing the first pinned ferromagnetic layer to a gas containing oxygen atoms at a pressure of 5 × 10 _7 Pa or more and 1 × 10 _4 Pa or less; 前記第 1固定強磁性層の上に第 2固定強磁性層を形成する工程と、  Forming a second pinned ferromagnetic layer on the first pinned ferromagnetic layer; 前記第 2固定強磁性層の上にトンネルバリア層を形成する工程と、  Forming a tunnel barrier layer on the second pinned ferromagnetic layer; 前記トンネルバリア層の上に自由強磁性層を形成する工程と  Forming a free ferromagnetic layer on the tunnel barrier layer; を具備する  With 磁気抵抗効果素子の製造方法。  Manufacturing method of magnetoresistive effect element. [2] 請求項 1に記載の磁気抵抗効果素子の製造方法にお!、て、 [2] In the method of manufacturing a magnetoresistive element according to claim 1,! 前記第 2固定強磁性層の膜厚は、 0より大きく lnm以下である  The film thickness of the second pinned ferromagnetic layer is greater than 0 and less than or equal to lnm 磁気抵抗効果素子の製造方法。  Manufacturing method of magnetoresistive effect element. [3] 基板の上面側に反強磁性層を形成する工程と、 [3] forming an antiferromagnetic layer on the upper surface side of the substrate; 前記反強磁性層の上に第 1固定強磁性層を形成する工程と、  Forming a first pinned ferromagnetic layer on the antiferromagnetic layer; 前記第 1固定強磁性層を 5 X 10_7Pa以上 1 X 10_4Pa未満の圧力で酸素原子を含 む気体に暴露を行う工程と、 Exposing the first pinned ferromagnetic layer to a gas containing oxygen atoms at a pressure of 5 × 10 _7 Pa or more and less than 1 × 10 _4 Pa; 前記第 1固定強磁性層の上にトンネルバリア層を形成する工程と、  Forming a tunnel barrier layer on the first pinned ferromagnetic layer; 前記トンネルバリア層の上に自由強磁性層を形成する工程と  Forming a free ferromagnetic layer on the tunnel barrier layer; を具備する  With 磁気抵抗効果素子の製造方法。  Manufacturing method of magnetoresistive effect element. [4] 基板の上面側に反強磁性層を形成する工程と、 [4] forming an antiferromagnetic layer on the upper surface side of the substrate; 前記反強磁性層の上に固定強磁性層を形成する工程と、  Forming a pinned ferromagnetic layer on the antiferromagnetic layer; 前記固定強磁性層の上にトンネルバリア層を含む膜を形成する工程と、 前記トンネルバリア層の上に自由強磁性層を形成する工程と  Forming a film including a tunnel barrier layer on the fixed ferromagnetic layer; forming a free ferromagnetic layer on the tunnel barrier layer; を具備し、  Comprising 前記トンネルバリア層を含む膜は、前記固定強磁性層との界面における前記トンネ ルバリア層の平均表面粗さより前記自由強磁性層との界面における前記トンネルバリ ァ層の平均表面粗さが小さくなるように形成される The film including the tunnel barrier layer has the tunnel barrier layer at the interface with the free ferromagnetic layer based on the average surface roughness of the tunnel barrier layer at the interface with the fixed ferromagnetic layer. The average surface roughness of the layer is formed to be small 磁気抵抗効果素子の製造方法。  Manufacturing method of magnetoresistive effect element. [5] 請求項 4に記載の磁気抵抗効果素子の製造方法にお 、て、 [5] In the method of manufacturing a magnetoresistive element according to claim 4, トンネルバリア層を含む膜を形成する工程は、  The step of forming a film including a tunnel barrier layer includes: 前記固定強磁性層を所定の雰囲気に暴露する工程と、  Exposing the pinned ferromagnetic layer to a predetermined atmosphere; 前記暴露する工程の後、前記トンネルバリア層を形成する工程と  After the exposing step, forming the tunnel barrier layer; を具備する磁気抵抗効果素子の製造方法。  The manufacturing method of the magnetoresistive effect element which comprises this. [6] 請求項 4に記載の磁気抵抗効果素子の製造方法にお 、て、 [6] In the method of manufacturing a magnetoresistive element according to claim 4, トンネルバリア層を含む膜を形成する工程は、  The step of forming a film including a tunnel barrier layer includes: 前記固定強磁性層を所定の雰囲気に暴露する工程と、  Exposing the pinned ferromagnetic layer to a predetermined atmosphere; 前記暴露する工程の後、前記固定強磁性層の上に付加的強磁性層を形成するェ 程と、  After the exposing step, forming an additional ferromagnetic layer on the pinned ferromagnetic layer; 前記付加的強磁性層の上に前記トンネルバリア層を形成する工程と  Forming the tunnel barrier layer on the additional ferromagnetic layer; を具備する磁気抵抗効果素子の製造方法。  The manufacturing method of the magnetoresistive effect element which comprises this. [7] 請求項 6に記載の磁気抵抗効果素子の製造方法にお 、て、 [7] In the method of manufacturing a magnetoresistive element according to claim 6, 前記第 2固定強磁性層の膜厚は、 0より大きく lnm以下である  The film thickness of the second pinned ferromagnetic layer is greater than 0 and less than or equal to lnm 磁気抵抗効果素子の製造方法。  Manufacturing method of magnetoresistive effect element. [8] 請求項 5乃至 7に記載の磁気抵抗効果素子の製造方法において、 [8] In the method of manufacturing a magnetoresistive effect element according to claims 5 to 7, 前記固定強磁性層を所定の雰囲気に暴露する工程は、  Exposing the pinned ferromagnetic layer to a predetermined atmosphere, 前記固定強磁性層を、 5 X 10_7Pa以上 1 X 10_4Pa未満の圧力で酸素原子を含 む気体に暴露を行う工程 Exposing the pinned ferromagnetic layer to a gas containing oxygen atoms at a pressure of 5 × 10 _7 Pa or more and less than 1 × 10 _4 Pa を具備する磁気抵抗効果素子の製造方法。  The manufacturing method of the magnetoresistive effect element which comprises this. [9] 請求項 1から 3と 8の 、ずれか一項に記載の磁気抵抗効果素子の製造方法にお!、 て、 [9] In the method for manufacturing a magnetoresistive effect element according to any one of claims 1 to 3 and 8,! 前記第 1固定強磁性層を前記酸素原子を含む気体に暴露を行う工程は、 1 X 10_6Pa以上 1 X 10_5Pa以下の圧力で酸素原子を含む気体に暴露を行う 磁気抵抗効果素子の製造方法。 The step of the first fixed ferromagnetic layer performs exposure to a gas containing the oxygen atom to a magnetoresistive element for exposure to a gas containing 1 X 10 _6 Pa or more 1 X 10 _5 Pa or less oxygen atoms at a pressure Production method. [10] 請求項 1から 3、 8, 9のいずれか一項に記載の磁気抵抗効果素子の製造方法にお いて、 [10] The method of manufacturing a magnetoresistive element according to any one of claims 1 to 3, 8, and 9. And 前記酸素原子を含む気体は、酸素ガス、水、メタノール及びエタノールガスのうちの 少なくとも一つを含む気体である  The gas containing oxygen atoms is a gas containing at least one of oxygen gas, water, methanol, and ethanol gas. 磁気抵抗効果素子の製造方法。  Manufacturing method of magnetoresistive effect element. [11] 請求項 1乃至 10のいずれか一項に記載の磁気抵抗効果素子の製造方法におい て、  [11] In the method of manufacturing a magnetoresistive effect element according to any one of claims 1 to 10, 前記第 1固定強磁性層力 CoFe、 NiFe、 CoFeB、 CoFeCrのうちの一つを含む 膜を備える  The first fixed ferromagnetic layer force comprises a film containing one of CoFe, NiFe, CoFeB, and CoFeCr 磁気抵抗効果素子の製造方法。  Manufacturing method of magnetoresistive effect element. [12] 請求項 1乃至 11のいずれか一項に記載の磁気抵抗効果素子の製造方法におい て、 [12] In the method of manufacturing a magnetoresistive effect element according to any one of claims 1 to 11, 前記トンネルバリア層の前記第 1固定強磁性層側の表面粗さが、前記第 1固定強 磁性層より下層の表面粗さより小さい  The surface roughness of the tunnel barrier layer on the first pinned ferromagnetic layer side is smaller than the surface roughness of the lower layer than the first pinned ferromagnetic layer 磁気抵抗効果素子の製造方法。  Manufacturing method of magnetoresistive effect element. [13] 基板の上面側に形成された反強磁性層と、 [13] an antiferromagnetic layer formed on the upper surface side of the substrate; 前記反強磁性層の上に形成された第 1固定強磁性層と、  A first pinned ferromagnetic layer formed on the antiferromagnetic layer; 前記第 1固定強磁性層の上に形成された第 2固定強磁性層と、  A second pinned ferromagnetic layer formed on the first pinned ferromagnetic layer; 前記第 2固定強磁性層の上に形成されたトンネルバリア層と、  A tunnel barrier layer formed on the second pinned ferromagnetic layer; 前記トンネルバリア層の上に形成された自由強磁性層と  A free ferromagnetic layer formed on the tunnel barrier layer; を具備し、  Comprising 前記第 1固定強磁性層の前記第 2固定強磁性層側の表面の領域は、他の領域に 比較して酸素濃度が高ぐ  The region of the surface of the first pinned ferromagnetic layer on the second pinned ferromagnetic layer side has a higher oxygen concentration than other regions. 前記トンネルバリア層側の前記第 1固定強磁性層の表面粗さが、前記第 1固定強 磁性層より下層の表面粗さより小さい  The surface roughness of the first pinned ferromagnetic layer on the tunnel barrier layer side is smaller than the surface roughness of the layer below the first pinned ferromagnetic layer 磁気抵抗効果素子。  Magnetoresistive effect element. [14] 請求項 13に記載の磁気抵抗効果素子にお 、て、 [14] In the magnetoresistance effect element according to claim 13, 前記第 2固定強磁性層の膜厚は、 0より大きく lnm以下である  The film thickness of the second pinned ferromagnetic layer is greater than 0 and less than or equal to lnm 磁気抵抗効果素子。 Magnetoresistive effect element. [15] 基板の上面側に形成された反強磁性層と、 [15] an antiferromagnetic layer formed on the upper surface side of the substrate; 前記反強磁性層の上に形成された第 1固定強磁性層と、  A first pinned ferromagnetic layer formed on the antiferromagnetic layer; 前記第 1固定強磁性層の上に形成されたトンネルバリア層と、  A tunnel barrier layer formed on the first pinned ferromagnetic layer; 前記トンネルバリア層の上に形成された自由強磁性層と  A free ferromagnetic layer formed on the tunnel barrier layer; を具備し、  Comprising 前記トンネルバリア層側の前記第 1固定強磁性層の表面粗さが、前記第 1固定強 磁性層より下層の表面粗さより小さい  The surface roughness of the first pinned ferromagnetic layer on the tunnel barrier layer side is smaller than the surface roughness of the layer below the first pinned ferromagnetic layer 磁気抵抗効果素子。  Magnetoresistive effect element. [16] 請求項 13乃至 15のいずれか一項に記載の磁気抵抗効果素子において、  [16] The magnetoresistance effect element according to any one of claims 13 to 15, 前記第 1固定強磁性層力 CoFe、 NiFe、 CoFeB、 CoFeCrのうちの一つを含む 膜を備える  The first fixed ferromagnetic layer force comprises a film containing one of CoFe, NiFe, CoFeB, and CoFeCr 磁気抵抗効果素子。  Magnetoresistive effect element. [17] 第 1方向へ延伸する複数のワード線と、 [17] a plurality of word lines extending in the first direction; 第 1方向と実質的に垂直な第 2方向へ伸びる複数のビット線と、  A plurality of bit lines extending in a second direction substantially perpendicular to the first direction; 前記複数のワード線と前記複数のビット線との交点の各々に設けられ、請求項 13 乃至 16のいずれか一項に記載の複数の磁気抵抗効果素子と  The plurality of magnetoresistance effect elements according to any one of claims 13 to 16, provided at each of intersections of the plurality of word lines and the plurality of bit lines. を具備する磁気ランダムアクセスメモリ。  A magnetic random access memory comprising:
PCT/JP2005/012955 2004-07-14 2005-07-13 Magnetoresistive device, method for manufacturing magnetoresistive device and magnetic random access memory Ceased WO2006006630A1 (en)

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